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Updated branching fraction measurements of B0( s) → K0Sh+h′ − decays
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Abstract
The charmless three-body decays B
(
s)
0
→ K
S
0
h
+
h
′ − (where h
(′) = π, K) are analysed using a sample of pp collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 3 fb−1. The branching fractions are measured relative to that of the B
0 → K
S
0
π
+
π
− decay, and are determined to be:
$$ \begin{array}{l}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{\pi}^{-}\right)}=0.123\pm 0.009\left(\mathrm{stat}\right)\pm 0.015\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.549\pm 0.018\left(\mathrm{stat}\right)\pm 0.033\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.191\pm 0.027\left(\mathrm{stat}\right)\pm 0.031\left(\mathrm{syst}\right)\pm 0.011\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=1.70\pm 0.07\left(\mathrm{stat}\right)\pm 0.11\left(\mathrm{syst}\right)\pm 0.10\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}\in \left[0.008-0.051\right]\kern0.5em \mathrm{at}\kern0.5em 90\%\kern0.5em \mathrm{confidence}\kern0.5em \mathrm{level},\hfill \end{array} $$
ℬ
B
0
→
K
S
0
K
±
π
∓
ℬ
B
0
→
K
S
0
K
+
π
−
=
0.123
±
0.009
stat
±
0.015
syst
,
ℬ
B
0
→
K
S
0
K
+
K
−
ℬ
B
0
→
K
S
0
π
+
π
−
=
0.549
±
0.018
stat
±
0.033
syst
,
ℬ
B
s
0
→
K
S
0
π
+
π
−
ℬ
B
0
→
K
S
0
π
+
π
−
=
0.191
±
0.027
stat
±
0.031
syst
±
0.011
f
s
/
f
d
,
ℬ
B
s
0
→
K
S
0
K
±
π
∓
ℬ
B
0
→
K
S
0
π
+
π
−
=
1.70
±
0.07
stat
±
0.11
syst
±
0.10
f
s
/
f
d
,
ℬ
B
s
0
→
K
S
0
K
+
K
−
ℬ
B
0
→
K
S
0
π
+
π
−
∈
0.008
−
0.051
at
90
%
confidence
level
,
where f
s
/f
d
represents the ratio of hadronisation fractions of the B
s
0
and B
0 mesons.
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Y. Yao
H. Yin
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K. A. Zarebski
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Y. Zheng
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J. B. Zonneveld
S. Zucchelli
Title: Updated branching fraction measurements of B0(
s) → K0Sh+h′ − decays
Description:
Abstract
The charmless three-body decays B
(
s)
0
→ K
S
0
h
+
h
′ − (where h
(′) = π, K) are analysed using a sample of pp collision data recorded by the LHCb experiment, corresponding to an integrated luminosity of 3 fb−1.
The branching fractions are measured relative to that of the B
0 → K
S
0
π
+
π
− decay, and are determined to be:
$$ \begin{array}{l}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{\pi}^{-}\right)}=0.
123\pm 0.
009\left(\mathrm{stat}\right)\pm 0.
015\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.
549\pm 0.
018\left(\mathrm{stat}\right)\pm 0.
033\left(\mathrm{syst}\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=0.
191\pm 0.
027\left(\mathrm{stat}\right)\pm 0.
031\left(\mathrm{syst}\right)\pm 0.
011\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{\pm }{\pi}^{\mp}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}=1.
70\pm 0.
07\left(\mathrm{stat}\right)\pm 0.
11\left(\mathrm{syst}\right)\pm 0.
10\left({f}_s/{f}_d\right),\hfill \\ {}\frac{\mathrm{\mathcal{B}}\left({B}_s^0\to {K}_{\mathrm{S}}^0{K}^{+}{K}^{-}\right)}{\mathrm{\mathcal{B}}\left({B}^0\to {K}_{\mathrm{S}}^0{\pi}^{+}{\pi}^{-}\right)}\in \left[0.
008-0.
051\right]\kern0.
5em \mathrm{at}\kern0.
5em 90\%\kern0.
5em \mathrm{confidence}\kern0.
5em \mathrm{level},\hfill \end{array} $$
ℬ
B
0
→
K
S
0
K
±
π
∓
ℬ
B
0
→
K
S
0
K
+
π
−
=
0.
123
±
0.
009
stat
±
0.
015
syst
,
ℬ
B
0
→
K
S
0
K
+
K
−
ℬ
B
0
→
K
S
0
π
+
π
−
=
0.
549
±
0.
018
stat
±
0.
033
syst
,
ℬ
B
s
0
→
K
S
0
π
+
π
−
ℬ
B
0
→
K
S
0
π
+
π
−
=
0.
191
±
0.
027
stat
±
0.
031
syst
±
0.
011
f
s
/
f
d
,
ℬ
B
s
0
→
K
S
0
K
±
π
∓
ℬ
B
0
→
K
S
0
π
+
π
−
=
1.
70
±
0.
07
stat
±
0.
11
syst
±
0.
10
f
s
/
f
d
,
ℬ
B
s
0
→
K
S
0
K
+
K
−
ℬ
B
0
→
K
S
0
π
+
π
−
∈
0.
008
−
0.
051
at
90
%
confidence
level
,
where f
s
/f
d
represents the ratio of hadronisation fractions of the B
s
0
and B
0 mesons.
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Study of B+ c decays to the K+K−π+ final state by using B0 s , χc0 and D0 resonances and weak annihilation nonresonant topologys
A
bstract
In this research the weak decay of
B
...

