Abstract
The X(3872) is investigated by employing the quark-hadron hybrid model, that consists of the \(c\bar{c}\) core, \(D^{(*)}\bar{D}{}^*\), \(J/\psi \omega \), and \(J/\psi \rho \) two-meson states. Due to the attraction from the \(c\bar{c}\)-\(D\bar{D}{}^*\) coupling and from the OPEP tensor coupling, a very thin peak can appear at the \(D^{0}\bar{D}{}^{*0}\) threshold. The energy of the corresponding pole of the scattering matrix is \(E=+0.06-0.14i\) MeV, which is on the physical sheet and above the threshold, the same as the one of the poles from the LHCb data analysis.
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Acknowledgements
This work is supported in part by JSPS KAKENHI Grant Numbers JP16K05361 (S.T. and M.T.), JP20K14478 (Y.Y.), JP17K05441, Grants-in-Aid for Scientific Research on Innovative Areas (No. 18H05407) (A.H.), and RCNP-CORENet.
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Takeuchi, S., Yamaguchi, Y., Hosaka, A. et al. X(3872) Revisited: The Roles of OPEP and the Quark Degrees of Freedom. Few-Body Syst 62, 77 (2021). https://doi.org/10.1007/s00601-021-01663-8
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DOI: https://doi.org/10.1007/s00601-021-01663-8