Observation of $ψ(3686) \to Ω^- K^+ \barΞ^0 $+c.c Article Swipe
Related Concepts
Omega
Physics
Bar (unit)
Excited state
Branching fraction
Analytical Chemistry (journal)
Baryon
Nuclear physics
Chemistry
Chromatography
Meteorology
Quantum mechanics
BESIII Collaboration
,
F. De Mori
,
,
P. Adlarson
,
O. Afedulidis
,
X. Ai
,
R. Aliberti
,
A. Amoroso
,
Q. An
,
Y. Bai
,
O. Bakina
,
I. Balossino
,
Y. Ban
,
H. -R. Bao
,
V. Batozskaya
,
K. Begzsuren
,
N. Berger
,
M. Berlowski
,
M. Bertani
,
D. Bettoni
,
F. Bianchi
,
E. Bianco
,
A. Bortone
,
I. Boyko
,
R. A. Briere
,
A. Brueggemann
,
H. Cai
,
X. Cai
,
A. Calcaterra
,
G. F. Cao
,
N. Cao
,
S. A. Çetin
,
J. F. Chang
,
G. R. Che
,
G. Chelkov
,
Chen Chen
,
C. Chen
,
Chao Chen
,
Guihai Chen
,
H. S. Chen
,
H. Y. Chen
,
M. L. Chen
,
S. J. Chen
,
S. L. Chen
,
S. M. Chen
,
T. Chen
,
X. R. Chen
,
X. T. Chen
,
Y. B. Chen
,
Y. Q. Chen
,
Z. J. Chen
,
Z. Y. Chen
,
S. K. Choi
,
X. Chu
,
G. Cibinetto
,
F. Cossio
,
J. J. Cui
,
H. L. Dai
,
J. P. Dai
,
A. Dbeyssi
,
R. E. de Boer
,
D. Dedovich
,
C. Q. Deng
,
Z. Y. Deng
,
A. G. Denig
,
I. Denysenko
,
M. Destefanis
,
F. De Mori
,
B. Ding
,
X. X. Ding
,
Y. Ding
,
Y. Ding
,
J. Dong
,
L. Y. Dong
,
M. Y. Dong
,
X. Dong
,
M. C. Du
,
S. X. Du
,
Y. Y. Duan
,
Z. H. Duan
,
P. Egorov
,
Y. H. Fan
,
J. Fang
,
J. Fang
,
S. S. Fang
,
Wenxing Fang
,
Y. Fang
,
Y. Q. Fang
,
R. Farinelli
,
L. Fava
,
F. Feldbauer
,
G. Felici
,
C. Q. Feng
,
J. H. Feng
,
Y. T. Feng
,
M. Fritsch
,
C. D. Fu
,
J. Fu
,
Y. W. Fu
,
H. Gao
·
YOU?
·
· 2024
· Open Access
·
· DOI: https://doi.org/10.48550/arxiv.2401.08252
· OA: W4390962856
YOU?
·
· 2024
· Open Access
·
· DOI: https://doi.org/10.48550/arxiv.2401.08252
· OA: W4390962856
Using $(27.12 \pm 0.14) \times 10^{8}$ $ψ(3686)$ events collected with the BESIII detector at BEPCII, the decay of $ψ(3686) \to Ω^- K^+ \barΞ^0 +c.c.$ is observed for the first time. The branching fraction of this decay is measured to be $\mathcal{B}_{ψ(3686) \to Ω^- K^+ \barΞ^0 +c.c.}=(2.78 \pm 0.40 \pm 0.18 ) \times 10^{-6}$, where the first uncertainty is statistical and the second is systematic. Possible baryon excited states are searched for in this decay, but no evident intermediate state is observed with the current sample size.
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