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Heavy neutrino threshold effects in low energy phenomenology

Right handed neutrinos with mass of {\cal O} \; (10^{12}-10^{13}) GeV are required to implement the see-saw mechanism and generate neutrino masses capable of playing a role in structure formation. Moreover models of fermion masses often relate the Yukawa couplings involving these neutrinos to the up...

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Detalles Bibliográficos
Autores principales: Leontaris, G.K., Lola, S., Ross, Graham G.
Lenguaje:eng
Publicado: 1995
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(95)00377-5
http://cds.cern.ch/record/282464
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author Leontaris, G.K.
Lola, S.
Ross, Graham G.
author_facet Leontaris, G.K.
Lola, S.
Ross, Graham G.
author_sort Leontaris, G.K.
collection CERN
description Right handed neutrinos with mass of {\cal O} \; (10^{12}-10^{13}) GeV are required to implement the see-saw mechanism and generate neutrino masses capable of playing a role in structure formation. Moreover models of fermion masses often relate the Yukawa couplings involving these neutrinos to the up-quark Yukawa couplings. Here we study the effects of such couplings on the radiative corrections to quark masses. We find that b-\tau equality at M_{GUT} may still give the correct m_b/m_{\tau}-- ratio at low energies, but only if there is large \mu-\tau mixing in the charged leptonic sector. We propose specific mass matrix ``textures'' dictated by a U(1) family symmetry whose structure preserves m_b=m_{\tau} at M_{GUT}. In these schemes, due to the large \nu_{\mu} - \nu_{\tau} mixing, it is possible to give a simultaneous solution to the solar neutrino deficit and the atmospheric neutrino problem.
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institution Organización Europea para la Investigación Nuclear
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publishDate 1995
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spelling cern-2824642023-03-14T18:56:00Zdoi:10.1016/0550-3213(95)00377-5http://cds.cern.ch/record/282464engLeontaris, G.K.Lola, S.Ross, Graham G.Heavy neutrino threshold effects in low energy phenomenologyParticle Physics - PhenomenologyRight handed neutrinos with mass of {\cal O} \; (10^{12}-10^{13}) GeV are required to implement the see-saw mechanism and generate neutrino masses capable of playing a role in structure formation. Moreover models of fermion masses often relate the Yukawa couplings involving these neutrinos to the up-quark Yukawa couplings. Here we study the effects of such couplings on the radiative corrections to quark masses. We find that b-\tau equality at M_{GUT} may still give the correct m_b/m_{\tau}-- ratio at low energies, but only if there is large \mu-\tau mixing in the charged leptonic sector. We propose specific mass matrix ``textures'' dictated by a U(1) family symmetry whose structure preserves m_b=m_{\tau} at M_{GUT}. In these schemes, due to the large \nu_{\mu} - \nu_{\tau} mixing, it is possible to give a simultaneous solution to the solar neutrino deficit and the atmospheric neutrino problem.Right handed neutrinos with mass of ${\cal O} \; (10~{12}-10~{13})$ GeV are required to implement the see-saw mechanism and generate neutrino masses capable of playing a role in structure formation. Moreover models of fermion masses often relate the Yukawa couplings involving these neutrinos to the up-quark Yukawa couplings. Here we study the effects of such couplings on the radiative corrections to quark masses. We find that $b-\tau$ equality at $M_{GUT}$ may still give the correct $m_b/m_{\tau}$-- ratio at low energies, but only if there is large $\mu-\tau$ mixing in the charged leptonic sector. We propose specific mass matrix ``textures'' dictated by a $U(1)$ family symmetry whose structure preserves $m_b=m_{\tau}$ at $M_{GUT}$. In these schemes, due to the large $\nu_{\mu} - \nu_{\tau}$ mixing, it is possible to give a simultaneous solution to the solar neutrino deficit and the atmospheric neutrino problem.Right handed neutrinos with mass of ${\cal O} \; (10~{12}-10~{13})$ GeV are required to implement the see-saw mechanism and generate neutrino masses capable of playing a role in structure formation. Moreover models of fermion masses often relate the Yukawa couplings involving these neutrinos to the up-quark Yukawa couplings. Here we study the effects of such couplings on the radiative corrections to quark masses. We find that $b-\tau$ equality at $M_{GUT}$ may still give the correct $m_b/m_{\tau}$-- ratio at low energies, but only if there is large $\mu-\tau$ mixing in the charged leptonic sector. We propose specific mass matrix ``textures'' dictated by a $U(1)$ family symmetry whose structure preserves $m_b=m_{\tau}$ at $M_{GUT}$. In these schemes, due to the large $\nu_{\mu} - \nu_{\tau}$ mixing, it is possible to give a simultaneous solution to the solar neutrino deficit and the atmospheric neutrino problem.Right-handed neutrinos with mass of O (10 12 − 10 13 ) GeV are required to implement the see-saw mechanism and generate neutrino masses capable of playing a role in structure formation. Moreover models of fermion masses often relate the Yukawa couplings involving these neutrinos to the up-quark Yukawa couplings. Here we study the effects of such couplings on the radiative corrections to quark masses. We find that b − τ equality at M GUT may still give the correct m b / m τ -ratio at low energies, but only if there is large μ − τ mixing in the charged leptonic sector. We propose specific mass matrix “textures” dictated by a U (1) family symmetry whose structure preserves m b = m τ at M GUT . In these schemes, due to the large ν μ − ν τ mixing, it is possible to give a simultaneous solution to the solar neutrino deficit and the atmospheric neutrino problem.Right handed neutrinos with mass of ${\cal O} \; (10^{12}-10^{13})$ GeV are required to implement the see-saw mechanism and generate neutrino masses capable of playing a role in structure formation. Moreover models of fermion masses often relate the Yukawa couplings involving these neutrinos to the up-quark Yukawa couplings. Here we study the effects of such couplings on the radiative corrections to quark masses. We find that $b-\tau$ equality at $M_{GUT}$ may still give the correct $m_b/m_{\tau}$-- ratio at low energies, but only if there is large $\mu-\tau$ mixing in the charged leptonic sector. We propose specific mass matrix ``textures'' dictated by a $U(1)$ family symmetry whose structure preserves $m_b=m_{\tau}$ at $M_{GUT}$. In these schemes, due to the large $\nu_{\mu} - \nu_{\tau}$ mixing, it is possible to give a simultaneous solution to the solar neutrino deficit and the atmospheric neutrino problem.hep-ph/9505402CERN-TH-95-133HD-HEP-95-8IOA-95-323CERN-TH-95-133HD-HEP-95-8IOA-323oai:cds.cern.ch:2824641995-05-29
spellingShingle Particle Physics - Phenomenology
Leontaris, G.K.
Lola, S.
Ross, Graham G.
Heavy neutrino threshold effects in low energy phenomenology
title Heavy neutrino threshold effects in low energy phenomenology
title_full Heavy neutrino threshold effects in low energy phenomenology
title_fullStr Heavy neutrino threshold effects in low energy phenomenology
title_full_unstemmed Heavy neutrino threshold effects in low energy phenomenology
title_short Heavy neutrino threshold effects in low energy phenomenology
title_sort heavy neutrino threshold effects in low energy phenomenology
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0550-3213(95)00377-5
http://cds.cern.ch/record/282464
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AT lolas heavyneutrinothresholdeffectsinlowenergyphenomenology
AT rossgrahamg heavyneutrinothresholdeffectsinlowenergyphenomenology