Neutrino mixing and CP-violation

The prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: 1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; 2) three active plus one sterile neutrino when the LSND signal is also taken into acco...

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Detalles Bibliográficos
Autores principales: Donini, A., Gavela, M.B., Hernandez, P., Rigolin, S.
Lenguaje:eng
Publicado: 1999
Materias:
Particle Physics - Phenomenology
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(00)00029-8
http://cds.cern.ch/record/398912
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author Donini, A.
Gavela, M.B.
Hernandez, P.
Rigolin, S.
author_facet Donini, A.
Gavela, M.B.
Hernandez, P.
Rigolin, S.
author_sort Donini, A.
collection CERN
description The prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: 1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; 2) three active plus one sterile neutrino when the LSND signal is also taken into account. For the latter we develop one and two mass dominance approximations. The appearance of wrong sign muons in long baseline experiments and tau leptons in short baseline ones provides the best tests of CP-violation in scenarios 1) and 2), respectively.
id cern-398912
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1999
record_format invenio
spelling cern-3989122023-03-14T18:50:12Zdoi:10.1016/S0550-3213(00)00029-8http://cds.cern.ch/record/398912engDonini, A.Gavela, M.B.Hernandez, P.Rigolin, S.Neutrino mixing and CP-violationParticle Physics - PhenomenologyThe prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: 1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; 2) three active plus one sterile neutrino when the LSND signal is also taken into account. For the latter we develop one and two mass dominance approximations. The appearance of wrong sign muons in long baseline experiments and tau leptons in short baseline ones provides the best tests of CP-violation in scenarios 1) and 2), respectively.The prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: 1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; 2) three active plus one sterile neutrino when the LSND signal is also taken into account. For the latter we develop one and two mass dominance approximations. The appearance of wrong sign muons in long baseline experiments and tau leptons in short baseline ones provides the best tests of CP-violation in scenarios 1) and 2), respectively.The prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: 1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; 2) three active plus one sterile neutrino when the LSND signal is also taken into account. For the latter we develop one and two mass dominance approximations. The appearance of wrong sign muons in long baseline experiments and tau leptons in short baseline ones provides the best tests of CP-violation in scenarios 1) and 2), respectively.The prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: 1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; 2) three active plus one sterile neutrino when the LSND signal is also taken into account. For the latter we develop one and two mass dominance approximations. The appearance of wrong sign muons in long baseline experiments and tau leptons in short baseline ones provides the best tests of CP-violation in scenarios 1) and 2), respectively.The prospects of measuring the leptonic angles and CP-odd phases at a neutrino factory are discussed in two scenarios: (1) three active neutrinos as indicated by the present ensemble of atmospheric plus solar data; (2) three active plus one sterile neutrino when the LSND signal is also taken into account. For the latter we develop one and two mass dominance approximations. The appearance of wrong sign muons in long baseline experiments and tau leptons in short baseline ones provides the best tests of CP-violation in scenarios (1) and (2), respectively.hep-ph/9909254CERN-TH-99-252FTUAM-99-25FTUV-99-59IFIC-99-62CERN-TH-99-252FTUAM-99-25FTUV-99-59IFIC-99-62oai:cds.cern.ch:3989121999-09-07
spellingShingle Particle Physics - Phenomenology
Donini, A.
Gavela, M.B.
Hernandez, P.
Rigolin, S.
Neutrino mixing and CP-violation
title Neutrino mixing and CP-violation
title_full Neutrino mixing and CP-violation
title_fullStr Neutrino mixing and CP-violation
title_full_unstemmed Neutrino mixing and CP-violation
title_short Neutrino mixing and CP-violation
title_sort neutrino mixing and cp-violation
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(00)00029-8
http://cds.cern.ch/record/398912
work_keys_str_mv AT doninia neutrinomixingandcpviolation
AT gavelamb neutrinomixingandcpviolation
AT hernandezp neutrinomixingandcpviolation
AT rigolins neutrinomixingandcpviolation

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