Measurement of the branching fractions of B¯ → D()K−KS∗0 and B¯ → D()Ds− decays at Belle II
We present measurements of the branching fractions of eight B ¯ 0 → D (*)+ K − K S ∗ 0 , B − → D (*)0 K − K S ∗ 0 decay channels. The results are based on data from SuperKEKB electron-positron collisions at the Υ(4 S ) resonance collected with the Belle II detector, corresponding to an integrated lu...
Gespeichert in:
Veröffentlicht in: | The journal of high energy physics 2024-08, Vol.2024 (8), p.206 |
---|---|
Hauptverfasser: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | We present measurements of the branching fractions of eight
B
¯
0
→
D
(*)+
K
−
K
S
∗
0
,
B
−
→
D
(*)0
K
−
K
S
∗
0
decay channels. The results are based on data from SuperKEKB electron-positron collisions at the Υ(4
S
) resonance collected with the Belle II detector, corresponding to an integrated luminosity of 362 fb
−
1
. The event yields are extracted from fits to the distributions of the difference between expected and observed
B
meson energy, and are efficiency-corrected as a function of
m
(
K
−
K
S
∗
0
) and
m
(
D
(*)
K
S
∗
0
) in order to avoid dependence on the decay model. These results include the first observation of
B
¯
0
→
D
+
K
−
K
S
0
,
B
−
→
D*
0
K
−
K
S
0
, and
B
¯
0
→
D*
+
K
−
K
S
0
decays and a significant improvement in the precision of the other channels compared to previous measurements. The helicity-angle distributions and the invariant mass distributions of the
K
−
K
S
∗
0
systems are compatible with quasi-two-body decays via a resonant transition with spin-parity
J
P
= 1
−
for the
K
−
K
S
0
systems and
J
P
= 1
+
for the
K
−
K*
0
systems. We also present measurements of the branching fractions of four
B
¯
0
→
D
(*)+
D
s
−
,
B
−
→
D
(*)0
D
s
−
decay channels with a precision compatible to the current world averages. |
---|---|
ISSN: | 1029-8479 |
DOI: | 10.1007/JHEP08(2024)206 |