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Production of Excited Doubly Heavy Baryons at the Super-
Z
Z
Z
Factory
Authors
Huan-Yu Bi
Jing-Bo Li
Hong-Hao Ma
Juan-Juan Niu
Publication date
24 May 2023
Publisher
View
on
arXiv
Abstract
In the framework of nonrelativistic QCD, the
P
P
P
-wave excited doubly heavy baryons are thoroughly studied via the channel
e
+
e
β
β
β¨
Q
Q
β²
β©
[
n
]
β
Ξ
Q
Q
β²
+
Q
β²
Λ
+
Q
Λ
e^{+} e^{-}\rightarrow \langle QQ^{\prime}\rangle[n] \rightarrow \Xi_{QQ^{\prime}} +\bar{Q^{\prime}} +\bar{Q}
e
+
e
β
β
β¨
Q
Q
β²
β©
[
n
]
β
Ξ
Q
Q
β²
β
+
Q
β²
Λ
β
+
Q
Λ
β
, which takes place at the collision energy
Z
Z
Z
-pole.
Q
(
β²
)
Q^{(\prime)}
Q
(
β²
)
represents
b
b
b
or
c
c
c
quark for the production of
Ξ
c
c
\Xi_{cc}
Ξ
cc
β
,
Ξ
b
c
\Xi_{bc}
Ξ
b
c
β
, and
Ξ
b
b
\Xi_{bb}
Ξ
bb
β
, respectively. All of the intermediate diquark states
β¨
Q
Q
β²
β©
[
n
]
\langle QQ'\rangle[n]
β¨
Q
Q
β²
β©
[
n
]
in
P
P
P
-wave,
β¨
c
c
β©
[
1
P
1
]
3
Λ
\langle cc\rangle[^{1}P_{1}]_{\mathbf{\bar 3}}
β¨
cc
β©
[
1
P
1
β
]
3
Λ
β
,
β¨
c
c
β©
[
3
P
J
]
6
\langle cc\rangle[^{3}P_{J}]_{\mathbf{6}}
β¨
cc
β©
[
3
P
J
β
]
6
β
,
β¨
b
c
β©
[
1
P
1
]
3
Λ
/
6
\langle bc\rangle[^{1}P_{1}]_{\mathbf{\bar 3}/ \mathbf{6}}
β¨
b
c
β©
[
1
P
1
β
]
3
Λ
/
6
β
,
β¨
b
c
β©
[
3
P
J
]
3
Λ
/
6
\langle bc\rangle[^{3}P_{J}]_{\mathbf{\bar 3}/ \mathbf{6}}
β¨
b
c
β©
[
3
P
J
β
]
3
Λ
/
6
β
,
β¨
b
b
β©
[
1
P
1
]
3
Λ
\langle bb \rangle[^{1}P_{1}]_{\mathbf{\bar 3}}
β¨
bb
β©
[
1
P
1
β
]
3
Λ
β
, and
β¨
b
b
β©
[
3
P
J
]
6
\langle bb\rangle[^{3}P_{J}]_{\mathbf{6}}
β¨
bb
β©
[
3
P
J
β
]
6
β
with
J
=
0
J=0
J
=
0
, 1, or 2, are taken into account. The cross sections and differential distributions, including the transverse momentum, rapidity, angular, and invariant mass, are discussed for the excited baryons production. The result is that the contributions of
Ξ
c
c
\Xi_{cc}
Ξ
cc
β
,
Ξ
b
c
\Xi_{bc}
Ξ
b
c
β
, and
Ξ
b
b
\Xi_{bb}
Ξ
bb
β
in
P
P
P
-wave are found to be 3.97
%
\%
%
, 5.08
%
\%
%
, and 5.89
%
\%
%
, respectively, compared to
S
S
S
-wave. Supposing that all
P
P
P
-wave excited states can decay into the ground state 100\%, the total events
N
Ξ
c
c
=
8.48
Γ
1
0
4
β
6
N_{\Xi_{cc}}=8.48 \times10^{4-6}
N
Ξ
cc
β
β
=
8.48
Γ
1
0
4
β
6
,
N
Ξ
b
c
=
2.26
Γ
1
0
5
β
7
N_{\Xi_{bc}}=2.26\times10^{5-7}
N
Ξ
b
c
β
β
=
2.26
Γ
1
0
5
β
7
, and
N
Ξ
b
b
=
4.12
Γ
1
0
3
β
5
N_{\Xi_{bb}}=4.12 \times10^{3-5}
N
Ξ
bb
β
β
=
4.12
Γ
1
0
3
β
5
would be produced at the Super-
Z
Z
Z
Factory with a high luminosity up to
L
β
1
0
34
β
36
c
m
β
2
s
β
1
{\cal L} \simeq 10^{34-36}{\rm cm}^{-2} {\rm s}^{-1}
L
β
1
0
34
β
36
cm
β
2
s
β
1
.Comment: 13 pages, 4 figures, 4 table
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Last time updated on 26/05/2023