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Partial-wave analysis of J / ψ → γ γ ϕ
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Using a sample of
∼
10
10
J
/
ψ
events collected by the BESIII detector at the BEPCII collider, a partial-wave analysis of the decay
γ
γ
ϕ
is performed to investigate the intermediate resonances in
J
/
ψ
→
γ
R
,
R
→
γ
ϕ
. Resonances including
f
1
(
1285
)
,
η
(
1405
)
,
f
1
(
1420
)
,
f
1
(
1510
)
,
f
2
(
1525
)
,
X
(
1835
)
,
f
2
(
1950
)
,
f
2
(
2010
)
,
f
0
(
2200
)
, and
η
c
have been detected with statistical significance greater than
5
σ
. The product branching fractions
B
(
J
/
ψ
→
γ
R
,
R
→
γ
ϕ
)
are reported, and the resonance parameters of
η
(
1405
)
and
X
(
1835
)
have been precisely determined. It seems likely that
η
(
1405
)
and
X
(
1835
)
act as the first—and second—excited states of
η
′
, respectively. The observation of
η
c
→
γ
ϕ
holds great significance for the in depth study of charmonium properties. No evidence of
η
(
1295
)
,
η
1
(
1855
)
or X(2370) is found. The measured upper limits of relevant branching fraction products do not conflict with theoretical expectations for X(2370) as a pseudoscalar glueball and
η
1
(
1855
)
as a hybrid state.
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Title: Partial-wave analysis of
J
/
ψ
→
γ
γ
ϕ
Description:
Using a sample of
∼
10
10
J
/
ψ
events collected by the BESIII detector at the BEPCII collider, a partial-wave analysis of the decay
γ
γ
ϕ
is performed to investigate the intermediate resonances in
J
/
ψ
→
γ
R
,
R
→
γ
ϕ
.
Resonances including
f
1
(
1285
)
,
η
(
1405
)
,
f
1
(
1420
)
,
f
1
(
1510
)
,
f
2
(
1525
)
,
X
(
1835
)
,
f
2
(
1950
)
,
f
2
(
2010
)
,
f
0
(
2200
)
, and
η
c
have been detected with statistical significance greater than
5
σ
.
The product branching fractions
B
(
J
/
ψ
→
γ
R
,
R
→
γ
ϕ
)
are reported, and the resonance parameters of
η
(
1405
)
and
X
(
1835
)
have been precisely determined.
It seems likely that
η
(
1405
)
and
X
(
1835
)
act as the first—and second—excited states of
η
′
, respectively.
The observation of
η
c
→
γ
ϕ
holds great significance for the in depth study of charmonium properties.
No evidence of
η
(
1295
)
,
η
1
(
1855
)
or X(2370) is found.
The measured upper limits of relevant branching fraction products do not conflict with theoretical expectations for X(2370) as a pseudoscalar glueball and
η
1
(
1855
)
as a hybrid state.
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