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The decay $b\to s\gamma$ and the charged Higgs boson mass without R-Parity
The experimental measurement of $B(b \to s\gamma)$ imposes important constraints on the charged Higgs boson mass in the MSSM. We show that by adding bilinear R--Parity violation (BRpV) in the tau sector, these bounds are relaxed. The bound on $m_{H^{\pm}}$ in the MSSM--BRpV model is $\gsim 200-250$...
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Lenguaje: | eng |
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1999
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Acceso en línea: | https://dx.doi.org/10.22323/1.002.0007 http://cds.cern.ch/record/392664 |
_version_ | 1780893778800803840 |
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author | Torrente-Lujan, E |
author_facet | Torrente-Lujan, E |
author_sort | Torrente-Lujan, E |
collection | CERN |
description | The experimental measurement of $B(b \to s\gamma)$ imposes important constraints on the charged Higgs boson mass in the MSSM. We show that by adding bilinear R--Parity violation (BRpV) in the tau sector, these bounds are relaxed. The bound on $m_{H^{\pm}}$ in the MSSM--BRpV model is $\gsim 200-250$ GeV for the the heavy squark limit. For lighter squarks, light charged Higgs bosons can be reconciled with $B(b \to s\gamma)$ only if there is also a light chargino. In the BRpV model if we impose $m_{\chi^{\pm}_1}>90$ GeV $m_{H^{\pm}} bosons would be observable at LEP II. The relaxation of the bounds is due mainly to the fact that charged Higgs bosons mix with staus and they contribute importantly to $B(b \to s\gamma)$. |
id | cern-392664 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1999 |
record_format | invenio |
spelling | cern-3926642019-09-30T06:29:59Zdoi:10.22323/1.002.0007http://cds.cern.ch/record/392664engTorrente-Lujan, EThe decay $b\to s\gamma$ and the charged Higgs boson mass without R-ParityParticle Physics - PhenomenologyThe experimental measurement of $B(b \to s\gamma)$ imposes important constraints on the charged Higgs boson mass in the MSSM. We show that by adding bilinear R--Parity violation (BRpV) in the tau sector, these bounds are relaxed. The bound on $m_{H^{\pm}}$ in the MSSM--BRpV model is $\gsim 200-250$ GeV for the the heavy squark limit. For lighter squarks, light charged Higgs bosons can be reconciled with $B(b \to s\gamma)$ only if there is also a light chargino. In the BRpV model if we impose $m_{\chi^{\pm}_1}>90$ GeV $m_{H^{\pm}} bosons would be observable at LEP II. The relaxation of the bounds is due mainly to the fact that charged Higgs bosons mix with staus and they contribute importantly to $B(b \to s\gamma)$.hep-ph/9907220IFIC-99-233FTUV-99-23oai:cds.cern.ch:3926641999-07-06 |
spellingShingle | Particle Physics - Phenomenology Torrente-Lujan, E The decay $b\to s\gamma$ and the charged Higgs boson mass without R-Parity |
title | The decay $b\to s\gamma$ and the charged Higgs boson mass without R-Parity |
title_full | The decay $b\to s\gamma$ and the charged Higgs boson mass without R-Parity |
title_fullStr | The decay $b\to s\gamma$ and the charged Higgs boson mass without R-Parity |
title_full_unstemmed | The decay $b\to s\gamma$ and the charged Higgs boson mass without R-Parity |
title_short | The decay $b\to s\gamma$ and the charged Higgs boson mass without R-Parity |
title_sort | decay $b\to s\gamma$ and the charged higgs boson mass without r-parity |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.22323/1.002.0007 http://cds.cern.ch/record/392664 |
work_keys_str_mv | AT torrentelujane thedecaybtosgammaandthechargedhiggsbosonmasswithoutrparity AT torrentelujane decaybtosgammaandthechargedhiggsbosonmasswithoutrparity |