Abstract

Inspired by the recent observation of exotic resonances $X(4140)$, $X(4274)$, $X(4350)$, $X(4500)$, and $X(4700)$ reported by several experiment collaborations, we investigated the four-quark system $cs\overline{c}\overline{s}$ with quantum numbers ${J}^{PC}={1}^{++}$ and ${0}^{++}$ in the framework of the chiral quark model. Two configurations, diquark-antidiquark and meson-meson, with all possible color structures are considered. The results show that no molecular state can be formed, but the resonance may exist if the color structure of the meson-meson configuration is $8\ensuremath{\bigotimes}8$. In the present calculation, the $X(4274)$ can be assigned as the $cs\overline{c}\overline{s}$ tetraquark states with ${J}^{PC}={1}^{++}$, but the energy of $X(4140)$ is too low to be regarded as the tetraquark state. $X(4350)$ can be a good candidate of the compact tetraquark state with ${J}^{PC}={0}^{++}$. When the radial excitation is taken into account, the $X(4700)$ can be explained as the $2S$ radial excited tetraquark state with ${J}^{PC}={0}^{++}$. As for $X(4500)$, there is no matching state in our calculation.

Highlights

  • Several exotic resonances were observed in the invariant mass distribution of J=ψφ

  • In 2009, the CDF Collaboration found the Xð4140Þ with mass M 1⁄4 4143.0 Æ 2.9 Æ 1.2 MeV and width Γ 1⁄4 11.7þ−68

  • Æ 0.7 MeV and width Γ 1⁄4 13þ−918 Æ 4 MeV was reported by the Belle Collaboration in the γγ → J=ψφ process, and the possible spin parity is JPC 1⁄4 0þþ or 2þþ [2]

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Summary

INTRODUCTION

Several exotic resonances were observed in the invariant mass distribution of J=ψφ. Based on the simple colormagnetic interaction model, possible ground cscs ̄ tetraquark states in the diquark-antidiquark configuration have been investigated, and the interpretation of Xð4500Þ and Xð4700Þ needs orbital (radial or angular) excitation [11]. It should be emphasized that most of these explanations do not agree with each other, and many of these investigations neglected the spin-orbital interaction when the orbital excitations were taken into account To see whether these exotic resonances can be described by cscs ̄ tetraquark systems with JPC 1⁄4 0þþ; 1þþ, we do a high-precision four-body calculation based on the framework of the chiral quark model, which describes the hadron spectra and hadron-hadron interaction well [19,20].

CHIRAL QUARK MODEL AND WAVE FUNCTIONS
NUMERICAL RESULTS AND DISCUSSIONS
CONCLUSIONS
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