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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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Bibliographic Details
Published in:The European physical journal. C, Particles and fields Particles and fields, 2022-03, Vol.82 (3)
Main Authors: Zhang, Ze-Yang, Zheng, Xu-Chang, Wu, Xing-Gang
Format: Article
Language:English
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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.
ISSN:1434-6044
1434-6052
DOI:10.1140/epjc/s10052-022-10212-4