Abstract

The compact tetraquark states with fully heavy quark contents $QQ\overline{Q}\overline{Q}$ are studied as the bound states of the diquark-antidiquark within the Bethe-Salpeter framework. The (anti)diquark masses and form factors used are the same as we calculated the doubly heavy baryons in a previous work. Under the instantaneous approximation, the three-dimensional (Bethe-)Salpeter equation of the tetraquarks is derived and solved numerically to obtain the corresponding mass spectra and wave functions of the tetraquarks with ${J}^{PC}={0}^{++}$, ${1}^{+\ensuremath{-}}$, and ${2}^{++}$. Our results show that the three ground states of $cc\overline{c}\overline{c}$ locate in the mass range of 6.4--6.5 GeV, and the $bb\overline{b}\overline{b}$ states in mass range of 19.2--19.3 GeV. The obtained relativistic wave functions naturally include the mixing effects from the possible $D$ (or $G$) partial waves, and then can be further used to do precise calculations of the tetraquark decays. Based on the obtained results, the LHCb's observation $X(6900)$ is less likely to be the ground states of compact $cc\overline{c}\overline{c}$ tetraquarks but might be the first or second excited states. In addition, a widely used propagatorlike form factor is also investigated and discussed.

Highlights

  • The quantum chromodynamics and the quark model allows the well-known traditional hadrons, such as the qq -type mesons and qqq-type baryons, and the exotic tetraquark states and the pentaquark baryons [1,2]

  • Before giving the numerical results of the mass spectra and wave functions, we specify the numerical values of the parameters first

  • The model parameters used in this work are kept the same with that we applied in previous meson and baryon calculations [26,31,36,37,38,39,40], a 1⁄4 e 1⁄4 2.7183; λ 1⁄4 0.21 GeV2; a1 1⁄4 a2 1⁄4 0.06 GeV; FIG. 3

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Summary

INTRODUCTION

The quantum chromodynamics and the quark model allows the well-known traditional hadrons, such as the qq -type mesons and qqq-type baryons, and the exotic tetraquark states and the pentaquark baryons [1,2]. In this work we would try to push the BSE framework further to study the fully heavy QQQ Qsystem and develop a precise and systematic approach to describe the compact tetraquark states This manuscript is organized as follows: in Sec. II the (Bethe-)Salpeter equation is derived in the perspective of the tetraquarks taken as the axial-vector diquark-antidiquark bound states; in Sec. III the Salpeter wave functions of the tetraquarks with JPC 1⁄4 0þþ, 1þ−, and 2þþ are constructed; in Sec. IV the obtained mass spectra and wave functions are given and discussed; a brief summary is presented

TETRAQUARKS AS THE BOUND STATES OF DIQUARK AND ANTIDIQUARK
Bethe-Salpeter equation of two vector bosons
Diquark form factors and tetraquark interaction kernel
BSE under the instantaneous approximation
BS WAVE FUNCTIONS OF THE TETRAQUARK STATES
NUMERICAL RESULTS AND DISCUSSIONS
SUMMARY
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