Theoretical analysis uncovers attractive J/psi-nucleon interactions, suggesting soft-gluon exchange predominates.
The low-energy J/ψ N scattering is of significant importance for various reasons. It is deeply interconnected with the hidden-charm Pc pentaquark states, provides insights into the role of gluons in nucleon structures, and is pertinent to the properties of J/ψ in nuclear medium. The scattering can occur through two distinct mechanisms: the coupled-channel mechanism involving open-charm meson-baryon intermediate states Λc D(*) and Σc(*) D(*), and the soft-gluon exchange mechanism. In this study, we investigate the S-wave J/ψ N scattering length arising from both mechanisms. Our findings indicate that both mechanisms lead to attractive interactions, yielding scattering lengths of [-10, -0.1] × 10⁻³ fm for the coupled-channel mechanism and $<-0.16$ fm for the soft-gluon exchange mechanism, respectively. Notably, the soft-gluon exchange mechanism produces a scattering length that is at least one order of magnitude larger than that from the coupled-channel mechanism, indicating its predominance. These findings can be corroborated through lattice calculations and will enhance our understanding of scattering processes that violate the Okubo-Zweig-Iizuka rule.
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Wu et al. (2025) studied this question.
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