Abstract

The nature of the recently discovered Z_cZc and Z_bZb structures is intriguing. Their charge forces its minimal quark content to be Q\bar Q q\bar qQQ‾qq‾ (where Q=\{c,b\}Q={c,b} and q=\{u,d\}q={u,d}). In this work we perform a molecular coupled-channels calculation of the I^G(J^{PC})=1^+(1^{+-})IG(JPC)=1+(1+−) charm and bottom sectors in the framework of a constituent quark model which satisfactorily describes a wide range of properties of (non-)conventional hadrons containing heavy quarks. All the relevant channels are included for each sector, i.e.: The D^{(\ast)}\bar D^{\ast}+h.c.D(*)D‾*+h.c., \pi J/\psiπJ/ψ and \rho\eta_cρηc channels for the Z_cZc and B^{(\ast)}B^{\ast}B(*)B* and \Upsilon(nS)\piΥ(nS)π (n=1,2,3n=1,2,3) channels for the Z_bZb analysis. Possible structures of these resonances will be discussed.

Highlights

  • The search of exotic structures in the heavy meson spectra, beyond the simplest qqstructure, is relatively recent

  • The Zc(4020) resonance, close to the D∗ D ∗ threshold, was discovered soon after at BESIII in the e+e− → π+π−hc channel with a mass of M = (4022.9 ± 0.8 ± 2.7) MeV/c2 and a width of Γ = (7.9 ± 2.7 ± 2.6) MeV [9]

  • In this work we explore the I G(J PC ) = 1+(1+−) charm and bottom sector in a coupledchannels scheme, including the closest meson-meson thresholds

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Summary

Introduction

The search of exotic structures in the heavy meson spectra, beyond the simplest qqstructure, is relatively recent. The so-called Zb(10610) and Zb(10650) where charged structures close to the BB∗ and B∗B∗ thresholds, respectively, spotted in the Υ (5S) → π+π−Υ (nS) reaction. Few years later, their charmonium partners arrived. The BESIII and Belle Collaborations discovered the Zc(3900) [6, 7], close to the DD ∗ threshold, in the π+π−J /ψ invariant mass spectrum of the e+e− → π+π−J /ψ process at s = 4.26 GeV. The Zc(4020) resonance, close to the D∗ D ∗ threshold, was discovered soon after at BESIII in the e+e− → π+π−hc channel with a mass of M = (4022.9 ± 0.8 ± 2.7) MeV/c2 and a width of Γ = (7.9 ± 2.7 ± 2.6) MeV [9]

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