Cargando…

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...

Descripción completa

Detalles Bibliográficos
Autores principales: Eeg, J.O., Hiorth, A., Polosa, A.D.
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.65.054030
http://cds.cern.ch/record/519122
_version_ 1780897753065324544
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