Abstract

Recently experimentalists have discovered several charged charmonium-like hadrons Zc+Z_c^+ with unconventional quark content cˉcdˉu\bar cc\bar d u. We perform a search for Zc+Z_c^+ with mass below 4.2 4.2~GeV in the channel IG(JPC)=1+(1+−)I^G(J^{PC})=1^+(1^{+-}) using lattice QCD. The major challenge is presented by the two-meson states J/ψ πJ/ψ\, π, ψ2Sπψ_{2S}π, ψ1Dπψ_{1D}π, DDˉ∗D\bar D^*, D∗Dˉ∗D^*\bar D^*, ηcρη_cρ that are inevitably present in this channel. The spectrum of eigenstates is extracted using a number of meson-meson and diquark-antidiquark interpolating fields. For our pion mass of 266~MeV we find all the expected two-meson states but no additional candidate for Zc+Z_c^+ below 4.2 4.2~GeV. Possible reasons for not seeing an additional eigenstate related to Zc+Z_c^+ are discussed. We also illustrate how a simulation incorporating interpolators with a structure resembling low-lying two-mesons states seems to render a Zc+Z_c^+ candidate, which is however not robust after further two-meson states around 4.2 4.2~GeV are implemented.

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