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The most precise measurement of the CP asymmetry in the decay B − → D − s D 0 has been reported by LHCb collaboration with the value of (−0.4 ± 0.5 ± 0.5)%. In this study, the CP violation in the decay B − → D − s D 0 has been calculated under the factorization approach. This decay mode includes current-current tree and penguin diagrams and their amplitudes are considered separately. In each of the tree and penguin amplitudes, the strong and weak phases have been introduced. The CP asymmetry has been calculated in this work to be (−0.35 ± 0.03)%. Finally, from the sum of the amplitudes, we have calculated the total amplitude and obtained comparable results with experimental value for the branching ratio of B − → D − s D 0 decay.
The most precise measurement of the the slope of the time-dependent asymmetry defined by the parameter
Δ
Y
f
(
f
=
K
+
K
−
,
π
+
π
−
), of the decay rates of
D
0
and
D
¯
0
mesons into the final states in the decays
D
0
→
K
+
K
−
and
D
0
→
π
+
π
−
were recently reported by LHCb collaboration with the values of
Δ
Y
K
+
K
−
=
(
−
2.3
±
1.5
±
0.3
)
×
1
0
−
4
and
Δ
Y
π
+
π
−
=
(
−
4.0
±
2.8
±
0.4
)
×
1
0
−
4
.
In this study, we have obtained
Δ
Y
K
+
K
−
=
(
−
2.27
±
1.12
)
×
1
0
−
4
and
Δ
Y
π
+
π
−
=
(
−
3.15
±
1.72
)
×
1
0
−
4
where
Δ
Y
constrains possible
CP
violation. The
CP
violation in the decays
D
0
→
K
+
K
−
and
D
0
→
π
+
π
−
have been calculated under the factorization approach. These decay modes include a current-current tree and penguin diagrams that their amplitudes are considered separately, by introducing strong and weak phases with the
δ
and
ϕ
parameters, respectively. We have obtained for both of decays
δ
1
=
0
∘
,
δ
2
=
(
90.04
±
0.01
)
∘
,
ϕ
1
=
0
∘
and
ϕ
2
=
(
68.48
±
1.55
)
∘
.
The
CP
asymmetries are calculated to be
A
CP
(
K
+
K
−
)
=
(
+
0.03
±
0.02
)
%
and
A
CP
(
π
+
π
−
)
=
(
+
0.03
±
0.01
)
%
at
μ
=
1
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