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Gluonic mechanism for $B \to D\eta'$
We present a calculation of the process B --> D eta' within a heavy-light chiral quark model. We assume that the eta' has a large gluonic component, and its coupling is described via the glue-glue-eta' effective vertex. The main contribution comes from the non-factorizable part of...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2001
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.65.054030 http://cds.cern.ch/record/519122 |
_version_ | 1780897753065324544 |
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author | Eeg, J.O. Hiorth, A. Polosa, A.D. |
author_facet | Eeg, J.O. Hiorth, A. Polosa, A.D. |
author_sort | Eeg, J.O. |
collection | CERN |
description | We present a calculation of the process B --> D eta' within a heavy-light chiral quark model. We assume that the eta' has a large gluonic component, and its coupling is described via the glue-glue-eta' effective vertex. The main contribution comes from the non-factorizable part of the effective weak Lagrangian at quark level. We find, within our model-dependent assumptions, a branching ratio Br(B --> D eta') = (1.7 -- 3.3) 10^(-4), somewhat below the experimental upper bound 9.4 10^(-4). |
id | cern-519122 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2001 |
record_format | invenio |
spelling | cern-5191222023-03-14T19:54:25Zdoi:10.1103/PhysRevD.65.054030http://cds.cern.ch/record/519122engEeg, J.O.Hiorth, A.Polosa, A.D.Gluonic mechanism for $B \to D\eta'$Particle Physics - PhenomenologyWe present a calculation of the process B --> D eta' within a heavy-light chiral quark model. We assume that the eta' has a large gluonic component, and its coupling is described via the glue-glue-eta' effective vertex. The main contribution comes from the non-factorizable part of the effective weak Lagrangian at quark level. We find, within our model-dependent assumptions, a branching ratio Br(B --> D eta') = (1.7 -- 3.3) 10^(-4), somewhat below the experimental upper bound 9.4 10^(-4).We present a calculation of the process B --> D eta' within a heavy-light chiral quark model. We assume that the eta' has a large gluonic component, and its coupling is described via the glue-glue-eta' effective vertex. The main contribution comes from the non-factorizable part of the effective weak Lagrangian at quark level. We find, within our model-dependent assumptions, a branching ratio Br(B --> D eta') = (1.7 -- 3.3) 10^(-4), somewhat below the experimental upper bound 9.4 10^(-4).hep-ph/0109201CERN-TH-2001-250OSLO-TP-6-01HIP-2001-49-THCERN-TH-2001-250OSLO-TP-2001-6HIP-2001-049-THoai:cds.cern.ch:5191222001-09-21 |
spellingShingle | Particle Physics - Phenomenology Eeg, J.O. Hiorth, A. Polosa, A.D. Gluonic mechanism for $B \to D\eta'$ |
title | Gluonic mechanism for $B \to D\eta'$ |
title_full | Gluonic mechanism for $B \to D\eta'$ |
title_fullStr | Gluonic mechanism for $B \to D\eta'$ |
title_full_unstemmed | Gluonic mechanism for $B \to D\eta'$ |
title_short | Gluonic mechanism for $B \to D\eta'$ |
title_sort | gluonic mechanism for $b \to d\eta'$ |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1103/PhysRevD.65.054030 http://cds.cern.ch/record/519122 |
work_keys_str_mv | AT eegjo gluonicmechanismforbtodeta AT hiortha gluonicmechanismforbtodeta AT polosaad gluonicmechanismforbtodeta |