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The analysis of the charmonium-like states
X
∗
(
3860
)
X^{*}(3860)
X
∗
(
3860
)
,
X
(
3872
)
X(3872)
X
(
3872
)
,
X
(
3915
)
X(3915)
X
(
3915
)
,
X
(
3930
)
X(3930)
X
(
3930
)
and
X
(
3940
)
X(3940)
X
(
3940
)
according to its strong decay behaviors
Authors
Zhen Yu Li
Zhi Gang Wang
Guo Liang Yu
Publication date
9 May 2017
Publisher
'IOP Publishing'
Doi
Cite
View
on
arXiv
Abstract
Inspired by the newly observed state
X
∗
(
3860
)
X^{*}(3860)
X
∗
(
3860
)
, we analyze the strong decay behaviors of some charmonium-like states
X
∗
(
3860
)
X^{*}(3860)
X
∗
(
3860
)
,
X
(
3872
)
X(3872)
X
(
3872
)
,
X
(
3915
)
X(3915)
X
(
3915
)
,
X
(
3930
)
X(3930)
X
(
3930
)
and
X
(
3940
)
X(3940)
X
(
3940
)
by the
3
P
0
^{3}P_{0}
3
P
0
model. We carry out our work based on the hypothesis that these states are all being the charmonium systems. Our analysis indicates that
0
+
+
0^{++}
0
++
charmonium state can be a good candidate for
X
∗
(
3860
)
X^{*}(3860)
X
∗
(
3860
)
and
1
+
+
1^{++}
1
++
state is the possible assignment for
X
(
3872
)
X(3872)
X
(
3872
)
. Considering as the
3
1
S
0
3^{1}S_{0}
3
1
S
0
state, the decay behavior of
X
(
3940
)
X(3940)
X
(
3940
)
is inconsistent with the experimental data. So, we can not assign
X
(
3940
)
X(3940)
X
(
3940
)
as the
3
1
S
0
3^{1}S_{0}
3
1
S
0
charmonium state by present work. Besides, our analysis imply that it is reasonable to assign
X
(
3915
)
X(3915)
X
(
3915
)
and
X
(
3930
)
X(3930)
X
(
3930
)
to be the same state,
2
+
+
2^{++}
2
++
. However, combining our analysis with that of Zhou~\cite{ZhouZY}, we speculate that
X
(
3915
)
X(3915)
X
(
3915
)
/
X
(
3930
)
X(3930)
X
(
3930
)
might not be a pure
c
c
‾
c\overline{c}
c
c
systems
Similar works
Full text
Available Versions
Crossref
See this paper in CORE
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info:doi/10.1088%2F1674-1137%2...
Last time updated on 03/05/2021
arXiv.org e-Print Archive
See this paper in CORE
Go to the repository landing page
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oai:arXiv.org:1704.06763
Last time updated on 19/06/2017