Abstract

The recently discovered fully charmed tetraquark candidate $X(6900)$ is analyzed within the frameworks of effective-range expansion, compositeness relation and width saturation, and a coupled multichannel dynamical study. By taking into account constraints from heavy-quark spin symmetry, the coupled-channel amplitude including the $J/\psi J/\psi,~ \chi_{c0}\chi_{c0}$ and $\chi_{c1}\chi_{c1}$ is constructed to fit the experimental di-$J/\psi$ event distributions around the energy region near $6.9$ GeV. Another dynamical two-coupled-channel amplitude with the $J/\psi J/\psi$ and $\psi(3770) J/\psi$ is also considered to describe the same datasets. The three different theoretical approaches lead to similar conclusions that the two-meson components do not play dominant roles in the $X(6900)$. Our determinations of the resonance poles in the complex energy plane from the refined coupled-channel study are found to be consistent with the experimental analyses. The coupled-channel amplitudes also have another pole corresponding to a narrow resonance $X(6825)$ that we predict sitting below the $\chi_{c0}\chi_{c0}$ threshold and of molecular origin. We give predictions to the line shapes of the $\chi_{c0}\chi_{c0}$ and $\chi_{c1}\chi_{c1}$ channels, which could provide a useful guide for future experimental measurements.

Highlights

  • The first fully heavy-flavor tetraquark meson candidate Xð6900Þ was recently observed in the di-J=ψ spectra by the LHCb Collaboration [1]

  • In this work we focus on the narrow peak named Xð6900Þ around 6.9 GeV observed in the J=ψJ=ψ event distributions from the LHCb measurements [1], which is the first discovered fully heavy-flavored tetraquark candidate

  • It is remarkable that different theoretical methods lead to similar conclusions for the

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Summary

INTRODUCTION

The first fully heavy-flavor tetraquark meson candidate Xð6900Þ was recently observed in the di-J=ψ spectra by the LHCb Collaboration [1]. In a series of recent works [3,4,5,6,7,8,9,10], we developed a theoretical framework that is especially useful for bringing insight into the inner structures of the resonance states near some underlying two-hadron thresholds It is based on the effective-range expansion (ERE) and the compositeness relation [3,10,11,12,13,14,15,16] and has been widely and successfully used to study many possible exotic hadrons, such as the charmed baryon Λcð2545Þ [4], the hidden bottom tetraquark candidates Zbð10610Þ=Zbð10650Þ [5], the narrow state Xð3872Þ [6], the pentaquark candidates Pcð4312Þ, Pcð4440Þ, Pcð4457Þ [8], and the hidden charm mesons Zcð3900Þ, Xð4020Þ, χc1ð4140Þ, ψð4260Þ, ψð4660Þ [7].

EFFECTIVE-RANGE EXPANSION FOR THE ELASTIC SCATTERING
80 Æ 38 168 Æ 77
Three-coupled-channel case
CONCLUSIONS

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