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Neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model
In the light of the recent muon (g_mu-2) result by the E821 experiment at the Brookhaven National Laboratory, we study the event rates of the charged lepton-flavour-violating (LFV) processes in the supersymmetric standard model (SUSY SM) with the heavy right-handed neutrinos (SUSY see-saw model). Si...
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Lenguaje: | eng |
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2001
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Acceso en línea: | https://dx.doi.org/10.1016/S0370-2693(01)00494-4 http://cds.cern.ch/record/489088 |
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author | Hisano, Junji Tobe, Kazuhiro |
author_facet | Hisano, Junji Tobe, Kazuhiro |
author_sort | Hisano, Junji |
collection | CERN |
description | In the light of the recent muon (g_mu-2) result by the E821 experiment at the Brookhaven National Laboratory, we study the event rates of the charged lepton-flavour-violating (LFV) processes in the supersymmetric standard model (SUSY SM) with the heavy right-handed neutrinos (SUSY see-saw model). Since the left-handed sleptons get the LFV masses via the neutrino Yukawa interaction in this model, the event rate of mu->e gamma and the SUSY-SM correction to (g_mu-2)/2 (a_mu(SUSY)) are strongly correlated. When the left-handed sleptons have a LFV mass between the first and second generations ((m^2_L)_{12}) in the mass matrix, it should be suppressed by \sim 10^{-3} (10^{-9}/a_mu(SUSY)) compared with the diagonal components (m_SUSY^2), from the current experimental bound on mu->e gamma. The recent (g_mu-2) result indicates a_mu(SUSY) \sim 10^{-9}. The future charged LFV experiments could cover (m^2_L)_{12}/m_SUSY^2 \gsim 10^{-(5-6)}. These experiments will give a significant impact on the flavour models and the SUSY-breaking models. In the typical models where the neutrino oscillation results are explained and the top quark and tau neutrino Yukawa couplings are unified at the GUT scale, a large LFV mass of (m^2_L)_{12}/m_SUSY^2 \gsim 10^{-4} is generated, and the large LFV event rates are predicted. We impose a so-called no-scale condition for the SUSY-breaking parameters at the GUT scale, which suppress the FCNC processes, and derive the conservative lower bound on mu-> e gamma. The predicted Br(mu-> e gamma) could be covered at the future LFV experiments. |
id | cern-489088 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2001 |
record_format | invenio |
spelling | cern-4890882023-03-12T06:01:25Zdoi:10.1016/S0370-2693(01)00494-4http://cds.cern.ch/record/489088engHisano, JunjiTobe, KazuhiroNeutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw modelParticle Physics - PhenomenologyIn the light of the recent muon (g_mu-2) result by the E821 experiment at the Brookhaven National Laboratory, we study the event rates of the charged lepton-flavour-violating (LFV) processes in the supersymmetric standard model (SUSY SM) with the heavy right-handed neutrinos (SUSY see-saw model). Since the left-handed sleptons get the LFV masses via the neutrino Yukawa interaction in this model, the event rate of mu->e gamma and the SUSY-SM correction to (g_mu-2)/2 (a_mu(SUSY)) are strongly correlated. When the left-handed sleptons have a LFV mass between the first and second generations ((m^2_L)_{12}) in the mass matrix, it should be suppressed by \sim 10^{-3} (10^{-9}/a_mu(SUSY)) compared with the diagonal components (m_SUSY^2), from the current experimental bound on mu->e gamma. The recent (g_mu-2) result indicates a_mu(SUSY) \sim 10^{-9}. The future charged LFV experiments could cover (m^2_L)_{12}/m_SUSY^2 \gsim 10^{-(5-6)}. These experiments will give a significant impact on the flavour models and the SUSY-breaking models. In the typical models where the neutrino oscillation results are explained and the top quark and tau neutrino Yukawa couplings are unified at the GUT scale, a large LFV mass of (m^2_L)_{12}/m_SUSY^2 \gsim 10^{-4} is generated, and the large LFV event rates are predicted. We impose a so-called no-scale condition for the SUSY-breaking parameters at the GUT scale, which suppress the FCNC processes, and derive the conservative lower bound on mu-> e gamma. The predicted Br(mu-> e gamma) could be covered at the future LFV experiments.In the light of the recent muon (g_mu-2) result by the E821 experiment at the Brookhaven National Laboratory, we study the event rates of the charged lepton-flavour-violating (LFV) processes in the supersymmetric standard model (SUSY SM) with the heavy right-handed neutrinos (SUSY see-saw model). Since the left-handed sleptons get the LFV masses via the neutrino Yukawa interaction in this model, the event rate of mu->e gamma and the SUSY-SM correction to (g_mu-2)/2 (\delta a_mu^{SUSY}) are strongly correlated. When the left-handed sleptons have a LFV mass between the first and second generations ((m^2_L)_{12}) in the mass matrix, it should be suppressed by \sim 10^{-3} ({10^-9}/\delta a_mu^{SUSY}) compared with the diagonal components (m_{SUSY}^2), from the current experimental bound on mu-> e gamma. The recent (g_mu-2) result indicates {\delta a_mu^{SUSY}}\sim 10^{-9}. The future charged LFV experiments could cover (m^2_L)_{12}/m_{SUSY}^2\gsim 10^{-(5-6)}. These experiments will give a significant impact on the flavour models and the SUSY-breaking models. In the SUSY see-saw model (m^2_L)_{12} is proportional to square of the tau-neutrino Yukawa-coupling constant. In the typical models where the neutrino-oscillation results are explained and the top-quark and tau-neutrino Yukawa couplings are unified at the GUT scale, a large LFV mass of (m^2_L)_{12}/m_{SUSY}^2\gsim 10^{-4} is generated, and the large LFV event rates are predicted. We impose a so-called no-scale condition for the SUSY-breaking parameters at the GUT scale, which suppresses the FCNC processes, and derive the conservative lower bound on mu-> egamma. The predicted Br(mu-> e gamma) could be covered at the future LFV experiments.In the light of the recent muon ( g μ −2) result by the E821 experiment at the Brookhaven National Laboratory, we study the event rates of the charged lepton-flavour-violating (LFV) processes in the supersymmetric standard model (SUSY SM) with the heavy right-handed neutrinos (SUSY see-saw model). Since the left-handed sleptons get the LFV masses via the neutrino Yukawa interaction in this model, the event rate of μ → eγ and the SUSY-SM correction to ( g μ −2)/2 ( δa μ SUSY ) are strongly correlated. When the left-handed sleptons have a LFV mass between the first and second generations ( (m 2 L ̃ ) 12 ) in the mass matrix, it should be suppressed by ∼10 −3 (10 −9 / δa μ SUSY ) compared with the diagonal components ( m SUSY 2 ), from the current experimental bound on μ → eγ . The recent ( g μ −2) result indicates δa μ SUSY ∼10 −9 . The future charged LFV experiments could cover (m 2 L ̃ ) 12 /m SUSY 2 ≳10 −(5 – 6) . These experiments will give a significant impact on the flavour models and the SUSY-breaking models. In the SUSY see-saw model (m 2 L ̃ ) 12 is proportional to square of the tau-neutrino Yukawa-coupling constant. In the typical models where the neutrino-oscillation results are explained and the top-quark and tau-neutrino Yukawa couplings are unified at the GUT scale, a large LFV mass of (m 2 L ̃ ) 12 /m SUSY 2 ≳10 −4 is generated, and the large LFV event rates are predicted. We impose a so-called no-scale condition for the SUSY-breaking parameters at the GUT scale, which suppresses the FCNC processes, and derive the conservative lower bound on μ → eγ . The predicted Br( μ → eγ ) could be covered at the future LFV experiments.hep-ph/0102315CERN-TH-2001-057KEK-TH-749CERN-TH-2001-057KEK-TH-749oai:cds.cern.ch:4890882001-02-26 |
spellingShingle | Particle Physics - Phenomenology Hisano, Junji Tobe, Kazuhiro Neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model |
title | Neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model |
title_full | Neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model |
title_fullStr | Neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model |
title_full_unstemmed | Neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model |
title_short | Neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model |
title_sort | neutrino masses, muon g-2, and lepton-flavour violation in the supersymmetric see-saw model |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/S0370-2693(01)00494-4 http://cds.cern.ch/record/489088 |
work_keys_str_mv | AT hisanojunji neutrinomassesmuong2andleptonflavourviolationinthesupersymmetricseesawmodel AT tobekazuhiro neutrinomassesmuong2andleptonflavourviolationinthesupersymmetricseesawmodel |