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The factorizable amplitude in $B^0 \to \pi^+ \pi^-$

Using the measured spectrum shape for $B \to \pi \ell \nu$, the rate for $B^+ \to \pi^+ \pi^0$, information on the Cabibbo-Kobayashi-Maskawa (CKM) matrix element $|V_{ub}|$, and theoretical inputs from factorization and lattice gauge theory, we obtain an improved estimate of the ``tree'' c...

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Detalles Bibliográficos
Autores principales: Luo, Z, Rosner, J L
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.68.074010
http://cds.cern.ch/record/618161
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author Luo, Z
Rosner, J L
author_facet Luo, Z
Rosner, J L
author_sort Luo, Z
collection CERN
description Using the measured spectrum shape for $B \to \pi \ell \nu$, the rate for $B^+ \to \pi^+ \pi^0$, information on the Cabibbo-Kobayashi-Maskawa (CKM) matrix element $|V_{ub}|$, and theoretical inputs from factorization and lattice gauge theory, we obtain an improved estimate of the ``tree'' contribution to $B^0 \to \pi^+ \pi^-$. We find the branching ratio $\b(B^0 \to \pi^+ \pi^-)|_{\rm tree} = (5.25^{+1.67}_{-0.50}) \times 10^{-6}$, to be compared with the experimental value $\b(B^0 \to \pi^+ \pi^-) = (4.55 \pm 0.44) \times 10^{-6}$. The fit implies $|V_{ub}| = (3.62 \pm 0.34) \times 10^{-3}$. Implications for tree-penguin interference in $B^0 \to \pi^+ \pi^-$ and for other charmless $B$ decays are discussed.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2003
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spelling cern-6181612019-09-30T06:29:59Zdoi:10.1103/PhysRevD.68.074010http://cds.cern.ch/record/618161engLuo, ZRosner, J LThe factorizable amplitude in $B^0 \to \pi^+ \pi^-$Particle Physics - PhenomenologyUsing the measured spectrum shape for $B \to \pi \ell \nu$, the rate for $B^+ \to \pi^+ \pi^0$, information on the Cabibbo-Kobayashi-Maskawa (CKM) matrix element $|V_{ub}|$, and theoretical inputs from factorization and lattice gauge theory, we obtain an improved estimate of the ``tree'' contribution to $B^0 \to \pi^+ \pi^-$. We find the branching ratio $\b(B^0 \to \pi^+ \pi^-)|_{\rm tree} = (5.25^{+1.67}_{-0.50}) \times 10^{-6}$, to be compared with the experimental value $\b(B^0 \to \pi^+ \pi^-) = (4.55 \pm 0.44) \times 10^{-6}$. The fit implies $|V_{ub}| = (3.62 \pm 0.34) \times 10^{-3}$. Implications for tree-penguin interference in $B^0 \to \pi^+ \pi^-$ and for other charmless $B$ decays are discussed.hep-ph/0305262EFI-2003-25-[CHICAGO]oai:cds.cern.ch:6181612003-05-23
spellingShingle Particle Physics - Phenomenology
Luo, Z
Rosner, J L
The factorizable amplitude in $B^0 \to \pi^+ \pi^-$
title The factorizable amplitude in $B^0 \to \pi^+ \pi^-$
title_full The factorizable amplitude in $B^0 \to \pi^+ \pi^-$
title_fullStr The factorizable amplitude in $B^0 \to \pi^+ \pi^-$
title_full_unstemmed The factorizable amplitude in $B^0 \to \pi^+ \pi^-$
title_short The factorizable amplitude in $B^0 \to \pi^+ \pi^-$
title_sort factorizable amplitude in $b^0 \to \pi^+ \pi^-$
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.68.074010
http://cds.cern.ch/record/618161
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