Observation of the decays χcJ → $$ {\mathrm{nK}}_{\mathrm{S}}^0\overline{\Lambda} $$ + c.c
A bstract By analyzing 4 . 48 × 10 8 ψ (3686) events collected with the BESIII detector, we observe the decays χ cJ → $$ {nK}_S^0\overline{\Lambda} $$ nK S 0 Λ ¯ + c . c . ( J = 0, 1, 2) for the first time, via the radiative transition ψ (3686) → γχ cJ . The branching fractions are determined to be...
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Published in: | The journal of high energy physics Vol. 2021; no. 11 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Journal Article |
Language: | English |
Published: |
01-11-2021
|
Online Access: | Get full text |
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Summary: | A
bstract
By analyzing 4
.
48 × 10
8
ψ
(3686) events collected with the BESIII detector, we observe the decays
χ
cJ
→
$$ {nK}_S^0\overline{\Lambda} $$
nK
S
0
Λ
¯
+ c
.
c
.
(
J
= 0, 1, 2) for the first time, via the radiative transition
ψ
(3686) →
γχ
cJ
. The branching fractions are determined to be (6
.
65 ± 0
.
26
stat
± 0
.
41
syst
) × 10
−
4
, (1
.
66 ± 0
.
12
stat
± 0
.
12
syst
) × 10
−
4
, and (3
.
58 ± 0
.
16
stat
± 0
.
23
syst
) × 10
−
4
for
J
= 0, 1, and 2, respectively. |
---|---|
ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP11(2021)217 |