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Charming Penguins in B decays

Full expressions of the $B^0_d \to \pi^+ \pi^-$ and $B^0_d \to \pi^0 \pi^0$ amplitudes, given in terms of matrix elements of operators of the effective weak Hamiltonian, are used to study the dependence of the relevant branching ratios on the different contributions. The uncertainty in the extractio...

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Detalles Bibliográficos
Autores principales: Ciuchini, Marco, Franco, E., Martinelli, G., Silvestrini, L.
Lenguaje:eng
Publicado: 1997
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(97)00388-X
http://cds.cern.ch/record/322608
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author Ciuchini, Marco
Franco, E.
Martinelli, G.
Silvestrini, L.
author_facet Ciuchini, Marco
Franco, E.
Martinelli, G.
Silvestrini, L.
author_sort Ciuchini, Marco
collection CERN
description Full expressions of the $B^0_d \to \pi^+ \pi^-$ and $B^0_d \to \pi^0 \pi^0$ amplitudes, given in terms of matrix elements of operators of the effective weak Hamiltonian, are used to study the dependence of the relevant branching ratios on the different contributions. The uncertainty in the extraction of the weak phase $\alpha$ from the measurement of the time-dependent asymmetry in $B^0_d \to \pi^+ \pi^-$ decays is also analyzed. We find that, among several effects which may enhance the $B^0_d \to \pi^0 \pi^0$ branching ratio, the most important is due to ``charming penguin" diagrams that have never been studied before. These diagrams easily increase $BR(B^0_d \to \pi^0 \pi^0)$ up to a value of $1-3 \times 10^{-6}$. The same effect produces, however, a large error in the extraction of $\alpha$ from the measurement of the $B^0_d \to charming-penguin amplitudes from the experimental measurement of many decay rates. Their effect is impressive in $B^+ \to \pi^+ K^0$ and $B^0_d \to K^+ $BR(B^+ \to \pi^+ K^0)$ and $BR(B^0_d \to K^+ \pi^-)$ of about $1 \times 10^{-5}$. Among other possibilities, we also suggest to use $B^0_d \to K^0 \bar K^0$, the BR of which can be as large as $2-3 \times 10^{-6}$, to determine the size of charming-penguin amplitudes.
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spelling cern-3226082022-08-05T02:28:44Zdoi:10.1016/S0550-3213(97)00388-Xhttp://cds.cern.ch/record/322608engCiuchini, MarcoFranco, E.Martinelli, G.Silvestrini, L.Charming Penguins in B decaysParticle Physics - PhenomenologyFull expressions of the $B^0_d \to \pi^+ \pi^-$ and $B^0_d \to \pi^0 \pi^0$ amplitudes, given in terms of matrix elements of operators of the effective weak Hamiltonian, are used to study the dependence of the relevant branching ratios on the different contributions. The uncertainty in the extraction of the weak phase $\alpha$ from the measurement of the time-dependent asymmetry in $B^0_d \to \pi^+ \pi^-$ decays is also analyzed. We find that, among several effects which may enhance the $B^0_d \to \pi^0 \pi^0$ branching ratio, the most important is due to ``charming penguin" diagrams that have never been studied before. These diagrams easily increase $BR(B^0_d \to \pi^0 \pi^0)$ up to a value of $1-3 \times 10^{-6}$. The same effect produces, however, a large error in the extraction of $\alpha$ from the measurement of the $B^0_d \to charming-penguin amplitudes from the experimental measurement of many decay rates. Their effect is impressive in $B^+ \to \pi^+ K^0$ and $B^0_d \to K^+ $BR(B^+ \to \pi^+ K^0)$ and $BR(B^0_d \to K^+ \pi^-)$ of about $1 \times 10^{-5}$. Among other possibilities, we also suggest to use $B^0_d \to K^0 \bar K^0$, the BR of which can be as large as $2-3 \times 10^{-6}$, to determine the size of charming-penguin amplitudes.Full expressions of the $B~0_d \to \pi~+ \pi~-$ and $B~0_d \to \pi~0 \pi~0$ amplitudes, given in terms of matrix elements of operators of the effective weak Hamiltonian, are used to study the dependence of the relevant branching ratios on the different contributions. The uncertainty in the extraction of the weak phase $\alpha$ from the measurement of the time-dependent asymmetry in $B~0_d \to \pi~+ \pi~-$ decays is also analyzed. We find that, among several effects which may enhance the $B~0_d \to \pi~0 \pi~0$ branching ratio, the most important is due to ``charming penguin" diagrams that have never been studied before. These diagrams easily increase $BR(B~0_d \to \pi~0 \pi~0)$ up to a value of $1-3 \times 10~{-6}$. The same effect produces, however, a large error in the extraction of $\alpha$ from the measurement of the $B~0_d \to \pi~+ \pi~-$ time-dependent asymmetry. We show that it is possible to determine charming-penguin amplitudes from the experimental measurement of many decay rates. Their effect is impressive in $B~+ \to \pi~+ K~0$ and $B~0_d \to K~+ \pi~-$ decays, where charming-penguin contributions easily give values of $BR(B~+ \to \pi~+ K~0)$ and $BR(B~0_d \to K~+ \pi~-)$ of about $1 \times 10~{-5}$. Among other possibilities, we also suggest to use $B~0_d \to K~0 \bar K~0$, the BR of which can be as large as $2-3 \times 10~{-6}$, to determine the size of charming-penguin amplitudes.Full expressions of the B d 0 → π + π − and B d 0 → π 0 π 0 amplitudes, given in terms of matrix elements of operators of the effective weak Hamiltonian, are used to study the dependence of the relevant branching ratios on the different contributions. The uncertainty in the extraction of the weak phase α from the measurement of the time-dependent asymmetry in B d 0 → π + π − decays is also analyzed. We find that, among several effects which may enhance the B d 0 → π 0 π 0 branching ratio, the most important is due to “charming penguin” diagrams. These diagrams easily increase BR( B d 0 → π 0 π 0 ) up to a value of 1−3 × 10 6 . The same effect produces, however, a large error in the extraction of a from the measurement of the B d 0 → π + π − time-dependent asymmetry. We show that it is possible to determine charming-penguin amplitudes from the experimental measurement of many decay rates. Their effect is impressive in B + → π + K 0 and B d 0 → K + π − decays, where charming-penguin contributions easily give values of BR( B + → π + K 0 ) and BR( B d 0 → K + π − ) of about 1 × 10 5 . Among other possibilities, we also suggest to use B d 0 → K 0 K 0 , the BR of which can be as large as 2−3 x 10 6 , to determine the size of charming-penguin amplitudes.Full expressions of the $B^0_d \to \pi^+ \pi^-$ and $B^0_d \to \pi^0 \pi^0$ amplitudes, given in terms of matrix elements of operators of the effective weak Hamiltonian, are used to study the dependence of the relevant branching ratios on the different contributions. The uncertainty in the extraction of the weak phase $\alpha$ from the measurement of the time-dependent asymmetry in $B^0_d \to \pi^+ \pi^-$ decays is also analyzed. We find that, among several effects which may enhance the $B^0_d \to \pi^0 \pi^0$ branching ratio, the most important is due to ``charming penguin" diagrams that have never been studied before. These diagrams easily increase $BR(B^0_d \to \pi^0 \pi^0)$ up to a value of $1-3 \times 10^{-6}$. The same effect produces, however, a large error in the extraction of $\alpha$ from the measurement of the $B^0_d \to \pi^+ \pi^-$ time-dependent asymmetry. We show that it is possible to determine charming-penguin amplitudes from the experimental measurement of many decay rates. Their effect is impressive in $B^+ \to \pi^+ K^0$ and $B^0_d \to K^+ \pi^-$ decays, where charming-penguin contributions easily give values of $BR(B^+ \to \pi^+ K^0)$ and $BR(B^0_d \to K^+ \pi^-)$ of about $1 \times 10^{-5}$. Among other possibilities, we also suggest to use $B^0_d \to K^0 \bar K^0$, the BR of which can be as large as $2-3 \times 10^{-6}$, to determine the size of charming-penguin amplitudes.hep-ph/9703353CERN-TH-97-030CERN-TH-97-30ROME-97-1168ROME-1168-1997ROM2F-97-09ROM2F--97-09CERN-TH-97-030ROM-2F-97-09ROMA-1-1168oai:cds.cern.ch:3226081997-03-19
spellingShingle Particle Physics - Phenomenology
Ciuchini, Marco
Franco, E.
Martinelli, G.
Silvestrini, L.
Charming Penguins in B decays
title Charming Penguins in B decays
title_full Charming Penguins in B decays
title_fullStr Charming Penguins in B decays
title_full_unstemmed Charming Penguins in B decays
title_short Charming Penguins in B decays
title_sort charming penguins in b decays
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(97)00388-X
http://cds.cern.ch/record/322608
work_keys_str_mv AT ciuchinimarco charmingpenguinsinbdecays
AT francoe charmingpenguinsinbdecays
AT martinellig charmingpenguinsinbdecays
AT silvestrinil charmingpenguinsinbdecays