$B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations

In this paper, a complete description of the channels $B \to V_1 V_2$ is given. Emphasis is put on the determination of the dynamical density matrix which elements are computed according to the Wilson operator product expansions entering into the formulation of the weak effective hamiltonian. \vskip...

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Detalles Bibliográficos
Autores principales: Ajaltouni, Z.J., Leitner, O., Rimbault, C.
Lenguaje:eng
Publicado: 2001
Materias:
Particle Physics - Phenomenology
Acceso en línea:http://cds.cern.ch/record/603989
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author Ajaltouni, Z.J.
Leitner, O.
Rimbault, C.
author_facet Ajaltouni, Z.J.
Leitner, O.
Rimbault, C.
author_sort Ajaltouni, Z.J.
collection CERN
description In this paper, a complete description of the channels $B \to V_1 V_2$ is given. Emphasis is put on the determination of the dynamical density matrix which elements are computed according to the Wilson operator product expansions entering into the formulation of the weak effective hamiltonian. \vskip 0.3cm Kinematical consequences related to the particular channel $B \to K^* {\rho}^0 (\omega)$ are described in details.
id cern-603989
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
record_format invenio
spelling cern-6039892023-03-14T19:49:09Zhttp://cds.cern.ch/record/603989engAjaltouni, Z.J.Leitner, O.Rimbault, C.$B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulationsParticle Physics - PhenomenologyIn this paper, a complete description of the channels $B \to V_1 V_2$ is given. Emphasis is put on the determination of the dynamical density matrix which elements are computed according to the Wilson operator product expansions entering into the formulation of the weak effective hamiltonian. \vskip 0.3cm Kinematical consequences related to the particular channel $B \to K^* {\rho}^0 (\omega)$ are described in details.In this paper, a complete description of the channels $B \to V_1 V_2$ is given. Emphasis is put on the determination of the dynamical density matrix which elements are computed according to the Wilson operator product expansions entering into the formulation of the weak effective hamiltonian. \vskip 0.3cm Kinematical consequences related to the particular channel $B \to K^* {\rho}^0 (\omega)$ are described in details.hep-ph/0302037LHCB-PHYS-2001-041ADP-01-11-T446PCCF-R1-01-04ADP-2001-11-T-446LHCb-PHYS-2001-041CERN-LHCb-PHYS-2001-041PCCF-RI-2001-04oai:cds.cern.ch:6039892001
spellingShingle Particle Physics - Phenomenology
Ajaltouni, Z.J.
Leitner, O.
Rimbault, C.
$B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations
title $B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations
title_full $B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations
title_fullStr $B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations
title_full_unstemmed $B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations
title_short $B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations
title_sort $b^0(\pm)$ decays into two vector mesons. physical motivations and a general method for simulations
topic Particle Physics - Phenomenology
url http://cds.cern.ch/record/603989
work_keys_str_mv AT ajaltounizj b0pmdecaysintotwovectormesonsphysicalmotivationsandageneralmethodforsimulations
AT leitnero b0pmdecaysintotwovectormesonsphysicalmotivationsandageneralmethodforsimulations
AT rimbaultc b0pmdecaysintotwovectormesonsphysicalmotivationsandageneralmethodforsimulations

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