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Production of the Bc meson at the CEPC
In this paper, we make a detailed study on the production of the B c , B c ∗ , B c ( 2 1 S 0 ) , and B c ∗ ( 2 3 S 1 ) mesons via the three planned running modes ( Z , W , and H ) at the future Circular Electron–Positron Collider (CEPC). The fragmentation-function and full nonrelativistic QCD approa...
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Published in: | The European physical journal. C, Particles and fields Particles and fields, 2022-03, Vol.82 (3) |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | In this paper, we make a detailed study on the production of the
B
c
,
B
c
∗
,
B
c
(
2
1
S
0
)
, and
B
c
∗
(
2
3
S
1
)
mesons via the three planned running modes (
Z
,
W
, and
H
) at the future Circular Electron–Positron Collider (CEPC). The fragmentation-function and full nonrelativistic QCD approaches are adopted to calculate the production cross sections. Considering the excited states shall decay to the ground
B
c
state (e.g.
1
1
S
0
-state) with almost
100
%
probability, our numerical results show that up to next-to-leading order QCD corrections, there are about
1.4
×
10
8
B
c
events to be accumulated via the
Z
mode (
s
=
m
Z
) of the CEPC, but only about
1.6
×
10
4
and
1.1
×
10
4
B
c
events to be accumulated via the
W
(
s
=
160
GeV
) and
H
(
s
=
240
GeV
) modes, respectively. Since the
Z
mode is the best mode among the three planned modes of the CEPC for studying the production of the
B
c
,
B
c
∗
,
B
c
(
2
1
S
0
)
, and
B
c
∗
(
2
3
S
1
)
mesons and the differential distributions of these mesons may be measured precisely at this mode, we further present the differential cross sections
d
σ
/
(
d
z
d
cos
θ
)
and
d
σ
/
d
z
via the
Z
mode of the CEPC. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-022-10212-4 |