Abstract

We consider a recent $T$-matrix analysis by Albaladejo {\it et al.}, [Phys.\ Lett.\ B {\bf 755}, 337 (2016)] which accounts for the $J/\psi\pi$ and $D^\ast\bar{D}$ coupled--channels dynamics, and that successfully describes the experimental information concerning the recently discovered $Z_c(3900)^\pm$. Within such scheme, the data can be similarly well described in two different scenarios, where the $Z_c(3900)$ is either a resonance or a virtual state. To shed light into the nature of this state, we apply this formalism in a finite box with the aim of comparing with recent Lattice QCD (LQCD) simulations. We see that the energy levels obtained for both scenarios agree well with those obtained in the single-volume LQCD simulation reported in Prelovsek {\it et al.} [Phys.\ Rev.\ D {\bf 91}, 014504 (2015)], making thus difficult to disentangle between both possibilities. We also study the volume dependence of the energy levels obtained with our formalism, and suggest that LQCD simulations performed at several volumes could help in discerning the actual nature of the intriguing $Z_c(3900)$ state.

Highlights

  • Since the discovery of the X (3872) in 2003 [1], the charmonium and charmonium-like spectrum are continuously being enlarged with new so-called X Y Z states [2,3,4], many of which do not fit properly in the conventional quark models [5]

  • We study the volume dependence of the energy levels obtained with our formalism and suggest that Lattice QCD (LQCD) simulations performed at several volumes could help in discerning the actual nature of the intriguing Zc(3900) state

  • The Zc(3900) structure is due to a resonance originating from the D∗ Dinteraction, while in the second one it is produced by the existence of a virtual state

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Summary

Introduction

Since the discovery of the X (3872) in 2003 [1], the charmonium and charmonium-like spectrum are continuously being enlarged with new so-called X Y Z states [2,3,4], many of which do not fit properly in the conventional quark models [5]. [35], which is the theoretical basis of the present manuscript, a J/ψπ –D∗ Dcoupled-channel scheme was proposed to describe the observed peaks associated to the Zc(3900), which is assumed to have I (J PC ) = 1(1+−) quantum numbers.1 Within this coupled-channel scheme, it was possible to successfully describe simultaneously the BESIII J ψπ [6] and D∗ D [10] invariant mass spectra, in which the Zc(3900)± structure has been seen. We will be able to compare the energy levels obtained with this finite volume T -matrix with those obtained in LQCD simulations, in particular those reported in Ref.

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