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Contribution of
b
→
s
g
g
b \to sgg
b
→
s
gg
through the QCD anomaly in exclusive decays
B
±
→
(
η
′
,
η
)
(
K
±
,
K
∗
±
)
B^{\pm}\to (\eta^{\prime},\eta)(K^{\pm}, K^{*\pm})
B
±
→
(
η
′
,
η
)
(
K
±
,
K
∗±
)
and
B
0
→
(
η
′
,
η
)
(
K
0
,
K
∗
0
)
B^{0}\to (\eta^{\prime},\eta)(K^{0},K^{*0})
B
0
→
(
η
′
,
η
)
(
K
0
,
K
∗
0
)
Authors
A. Ali
J. Chay
C. Greub
P. Ko
Publication date
1 January 1998
Publisher
'Elsevier BV'
Doi
Cite
View
on
arXiv
Abstract
We compute the decay rates for the exclusive decays
B
±
→
(
η
′
,
η
)
(
K
±
,
K
∗
±
)
B^{\pm} \to (\eta^{\prime},\eta) (K^{\pm}, K^{*\pm})
B
±
→
(
η
′
,
η
)
(
K
±
,
K
∗±
)
and
B
0
→
(
η
′
,
η
)
(
K
0
,
K
∗
0
)
B^{0}\to (\eta^{\prime},\eta) (K^{0}, K^{*0})
B
0
→
(
η
′
,
η
)
(
K
0
,
K
∗
0
)
in a QCD-improved factorization framework by including the contribution from the process
b
→
s
g
g
→
s
(
η
′
,
η
)
b\to sgg \to s (\eta^{\prime}, \eta)
b
→
s
gg
→
s
(
η
′
,
η
)
through the QCD anomaly. This method provides an alternative estimate of the contribution
b
→
s
c
c
ˉ
→
s
(
η
,
η
′
)
b \to s c\bar{c} \to s(\eta,\eta^\prime)
b
→
sc
c
ˉ
→
s
(
η
,
η
′
)
to these decays as compared to the one using the intrinsic charm content of the
η
′
\eta^{\prime}
η
′
and
η
\eta
η
mesons determined through the decays
J
/
ψ
→
(
η
,
η
′
,
η
c
)
γ
J/\psi \to (\eta,\eta^\prime ,\eta_c) \gamma
J
/
ψ
→
(
η
,
η
′
,
η
c
)
γ
. The resulting branching ratios are compared with the CLEO data on
B
±
→
η
′
K
±
B^{\pm} \to \eta^{\prime} K^{\pm}
B
±
→
η
′
K
±
and
B
0
→
η
′
K
0
B^{0} \to \eta^{\prime} K^{0}
B
0
→
η
′
K
0
and predictions are made for the rest.Comment: 16 pages including 4 postscript figures; uses epsfig. The most recent branching ratios from CLEO, ref. [5], are taken into account. The theory part is unchange
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DESY
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oai:bib-pubdb1.desy.de:331940
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info:doi/10.1016%2Fs0370-2693%...
Last time updated on 30/03/2021