Cargando…

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 $\gsim 200-250$...

Descripción completa

Detalles Bibliográficos
Autor principal: Torrente-Lujan, E
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.22323/1.002.0007
http://cds.cern.ch/record/392664
_version_ 1780893778800803840
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