A search for Bs0∗ and Bs1∗ through the K-p interaction.
Saved in:
| Title: | A search for Bs0∗ and Bs1∗ through the K-p interaction. |
|---|---|
| Authors: | Yuan, Min1 (AUTHOR) yuanm@my.swjtu.edu.cn, Huang, Yin1 (AUTHOR) huangy2019@swjtu.edu.cn |
| Source: | European Physical Journal C -- Particles & Fields. Mar2026, Vol. 86 Issue 3, p1-9. 9p. |
| Subjects: | Particle interactions, Nuclear cross sections, Heavy quark effective theory, Scattering (Physics), Mesons, Particle physics |
| Abstract: | Studying heavy-quark hadrons is crucial due to the nonperturbative nature of low-energy QCD, with Heavy-Quark Symmetry (HQS) serving as a key framework for understanding their spin and flavor symmetries. However, a key issue is that the theoretically expected B (∗) K ¯ molecular states have not yet been observed, although they are considered the bottom-quark counterparts of the observed D ¯ (∗) K ¯ molecular states (corresponding to D s 0 (2317 / 2460) - ), which challenges the universality of HQS. The main goal of this work is to search for the theoretically predicted B K ¯ and B ∗ K ¯ molecular states, namely B s 0 ∗ (5725) and B s 1 ∗ (5778) , via the reactions K - p → Λ b 0 B s 0 ∗ and K - p → Λ b 0 B s 1 ∗ . Within an effective Lagrangian framework, we compute the relevant cross sections, considering t-channel B (∗) exchanges and K - p initial-state interactions (ISI). The results show that the production cross sections of B s 0 ∗ (5725) and B s 1 ∗ (5778) can reach the order of 0.01 nb, and we suggest that experiments searching for B s 0 ∗ (5725) are best performed at P K - = 12.18 GeV , while higher energies are most favorable for producing B s 1 ∗ (5778) . The ISI play a crucial role, as they not only significantly enhance the production cross sections of B s 0 ∗ (5725) and B s 1 ∗ (5778) (by roughly one order of magnitude) but also markedly affect the angular distributions of the produced particles. We also calculated the production cross sections of the conventional quark–antiquark states B s 0 ∗ (5700) and B s 1 ∗ (5720) , which are found to be nearly the same as those of B s 0 ∗ (5725) and B s 1 ∗ (5778) . Although their internal structures remain ambiguous, these results can inform future experimental searches at CERN and J-PARC. [ABSTRACT FROM AUTHOR] |
| Copyright of European Physical Journal C -- Particles & Fields is the property of Springer Nature and its content may not be copied or emailed to multiple sites without the copyright holder's express written permission. Additionally, content may not be used with any artificial intelligence tools or machine learning technologies. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract. (Copyright applies to all Abstracts.) | |
| Database: | Engineering Source |
|
Full text is not displayed to guests.
Login for full access.
|
|
| Abstract: | Studying heavy-quark hadrons is crucial due to the nonperturbative nature of low-energy QCD, with Heavy-Quark Symmetry (HQS) serving as a key framework for understanding their spin and flavor symmetries. However, a key issue is that the theoretically expected B (∗) K ¯ molecular states have not yet been observed, although they are considered the bottom-quark counterparts of the observed D ¯ (∗) K ¯ molecular states (corresponding to D s 0 (2317 / 2460) - ), which challenges the universality of HQS. The main goal of this work is to search for the theoretically predicted B K ¯ and B ∗ K ¯ molecular states, namely B s 0 ∗ (5725) and B s 1 ∗ (5778) , via the reactions K - p → Λ b 0 B s 0 ∗ and K - p → Λ b 0 B s 1 ∗ . Within an effective Lagrangian framework, we compute the relevant cross sections, considering t-channel B (∗) exchanges and K - p initial-state interactions (ISI). The results show that the production cross sections of B s 0 ∗ (5725) and B s 1 ∗ (5778) can reach the order of 0.01 nb, and we suggest that experiments searching for B s 0 ∗ (5725) are best performed at P K - = 12.18 GeV , while higher energies are most favorable for producing B s 1 ∗ (5778) . The ISI play a crucial role, as they not only significantly enhance the production cross sections of B s 0 ∗ (5725) and B s 1 ∗ (5778) (by roughly one order of magnitude) but also markedly affect the angular distributions of the produced particles. We also calculated the production cross sections of the conventional quark–antiquark states B s 0 ∗ (5700) and B s 1 ∗ (5720) , which are found to be nearly the same as those of B s 0 ∗ (5725) and B s 1 ∗ (5778) . Although their internal structures remain ambiguous, these results can inform future experimental searches at CERN and J-PARC. [ABSTRACT FROM AUTHOR] |
|---|---|
| ISSN: | 14346044 |
| DOI: | 10.1140/epjc/s10052-026-15495-5 |