English

Tetraquark state $X(6900)$ and the interaction between diquark and antidiquark

High Energy Physics - Phenomenology 2021-06-15 v2 High Energy Physics - Experiment

Abstract

Recently LHCb declared a new structure X(6900)X(6900) in the final state di-J/ψJ/\psi which is popularly regarded as a cccc-cˉcˉ\bar c\bar c tetraquark state. %popularly. Within the Bethe-Salpeter (B-S) frame we study the possible cccc-cˉcˉ\bar c\bar c bound states and the interaction between diquark (cccc) and antidiquark (cˉcˉ\bar c\bar c). In this work cccc (cˉcˉ\bar c\bar c) is treated as a color anti-triplet (triplet) axial-vector so the quantum numbers of cccc-cˉcˉ\bar c\bar c bound state are 0+0^+, 1+1^+ and 2+2^+. Learning from the interaction in meson case and using the effective coupling we suggest the interaction kernel for diquark and antidiquark system. Then we deduce the B-S equations for different quantum numbers. Solving these equations numerically we find the spectra of some excited states can be close to the mass of X(6900)X(6900) when we assign appropriate values for parameter κ\kappa introduced in the interaction (kernel).We also briefly calculate the spectra of bbbb-bˉbˉ\bar b\bar b bound states. Future measurement of bbbb-bˉbˉ\bar b\bar b state will help us to determine the exact form of effective interaction.

Keywords

Cite

@article{arxiv.2103.13140,
  title  = {Tetraquark state $X(6900)$ and the interaction between diquark and antidiquark},
  author = {Hong-Wei Ke and Xin Han and Xiao-Hai Liu and Yan-Liang Shi},
  journal= {arXiv preprint arXiv:2103.13140},
  year   = {2021}
}

Comments

14 pages, two figures