The decay width of the Zc(3900)Z_c(3900) as an axialvector tetraquark state in solid quark–hadron duality

Nov 20, 2017
16 pages
Published in:
  • Eur.Phys.J.C 78 (2018) 1, 14
  • Published: Jan 11, 2018
e-Print:

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Abstract: (Springer)
In this article, we tentatively assign the Zc±(3900)Z_c^\pm (3900) to be the diquark–antidiquark type axialvector tetraquark state, study the hadronic coupling constants GZcJ/ψπ,GZcηcρ,GZcDDˉG_{Z_cJ/\psi \pi }, G_{Z_c\eta _c\rho }, G_{Z_cD \bar{D}^{*}} with the QCD sum rules in details. We take into account both the connected and disconnected Feynman diagrams in carrying out the operator product expansion, as the connected Feynman diagrams alone cannot do the work. Special attentions are paid to matching the hadron side of the correlation functions with the QCD side of the correlation functions to obtain solid duality, the routine can be applied to study other hadronic couplings directly. We study the two-body strong decays Zc+(3900)J/ψπ+,ηcρ+,D+Dˉ0,Dˉ0D+Z_c^+(3900)\rightarrow J/\psi \pi ^+, \eta _c\rho ^+, D^+ \bar{D}^{*0}, \bar{D}^0 D^{*+} and obtain the total width of the Zc±(3900)Z_c^\pm (3900) . The numerical results support assigning the Zc±(3900)Z_c^\pm (3900) to be the diquark–antidiquark type axialvector tetraquark state, and assigning the Zc±(3885)Z_c^\pm (3885) to be the meson–meson type axialvector molecular state.
Note:
  • 16 pages, 3 figures
  • tetraquark: axial-vector
  • quantum chromodynamics: sum rule
  • duality: quark hadron
  • correlation function
  • Feynman graph
  • operator product expansion
  • hadron: coupling constant
  • Z/c(3900)