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QCD factorization for exclusive, non-leptonic B decays

Exclusive, non-leptonic, two-body decays of B mesons simplify greatly in the heavy quark limit. In this talk I discuss the factorized structure that holds in this limit and some of its consequences: (a) naive factorization is recovered in a certain limit; (b) `non-factorizable' effects are hard...

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Autor principal: Beneke, M.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:http://cds.cern.ch/record/405410
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author Beneke, M.
author_facet Beneke, M.
author_sort Beneke, M.
collection CERN
description Exclusive, non-leptonic, two-body decays of B mesons simplify greatly in the heavy quark limit. In this talk I discuss the factorized structure that holds in this limit and some of its consequences: (a) naive factorization is recovered in a certain limit; (b) `non-factorizable' effects are hard and can be calculated; (c) strong interaction phases vanish in the heavy quark limit (and can be calculated as well). As an illustration, I compute the penguin contribution to the decay $B_d\to\pi^+\pi^-$ and its effect on the determination of $\sin 2\alpha$.
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institution Organización Europea para la Investigación Nuclear
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publishDate 1999
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spelling cern-4054102023-03-14T17:01:52Zhttp://cds.cern.ch/record/405410engBeneke, M.QCD factorization for exclusive, non-leptonic B decaysParticle Physics - PhenomenologyExclusive, non-leptonic, two-body decays of B mesons simplify greatly in the heavy quark limit. In this talk I discuss the factorized structure that holds in this limit and some of its consequences: (a) naive factorization is recovered in a certain limit; (b) `non-factorizable' effects are hard and can be calculated; (c) strong interaction phases vanish in the heavy quark limit (and can be calculated as well). As an illustration, I compute the penguin contribution to the decay $B_d\to\pi^+\pi^-$ and its effect on the determination of $\sin 2\alpha$.Exclusive, non-leptonic, two-body decays of B mesons simplify greatly in the heavy quark limit. In this talk I discuss the factorized structure that holds in this limit and some of its consequences: (a) naive factorization is recovered in a certain limit; (b) `non-factorizable' effects are hard and can be calculated; (c) strong interaction phases vanish in the heavy quark limit (and can be calculated as well). As an illustration, I compute the penguin contribution to the decay $B_d\to\pi^+\pi^-$ and its effect on the determination of $\sin 2\alpha$.hep-ph/9910505CERN-TH-99-319CERN-TH-99-319oai:cds.cern.ch:4054101999-10-28
spellingShingle Particle Physics - Phenomenology
Beneke, M.
QCD factorization for exclusive, non-leptonic B decays
title QCD factorization for exclusive, non-leptonic B decays
title_full QCD factorization for exclusive, non-leptonic B decays
title_fullStr QCD factorization for exclusive, non-leptonic B decays
title_full_unstemmed QCD factorization for exclusive, non-leptonic B decays
title_short QCD factorization for exclusive, non-leptonic B decays
title_sort qcd factorization for exclusive, non-leptonic b decays
topic Particle Physics - Phenomenology
url http://cds.cern.ch/record/405410
work_keys_str_mv AT benekem qcdfactorizationforexclusivenonleptonicbdecays