Abstract

Doubly heavy tetraquark states are the prime candidates for tightly bound exotic states. We present a systematic study of the mass spectra of the $S$-wave doubly heavy tetraquark states $QQ\bar{q}\bar{q}$ ($q=u, d, s$ and $Q=c, b$) with different quantum numbers $J^P=0^+$, $1^+$, and $2^+$ in the framework of the improved chromomagnetic interaction (ICMI) model. The parameters in the ICMI model are obtained by fitting the conventional hadron spectra and are used directly to predict the masses of the tetraquark states. For heavy quarks, the uncertainties of the parameters are obtained by comparing the masses of doubly and triply heavy baryons with those given by lattice QCD, QCD sum rules, and potential models. Several compact and stable bound states are found in both the doubly charmed and doubly bottomed tetraquark systems. The predicted mass of the $cc\bar u\bar d$ state is consistent with the recent measurement from the LHCb collaboration.

Highlights

  • Quantum chromodynamics (QCD) allows the existence of many fantastic hadrons, such as glueballs [1,2], hybrids [3,4], multiquark states [5,6], and hadronic molecules [7,8]

  • For triply heavy baryons with three identical heavy quarks, the total spin can only be S 1⁄4 3=2 and the mass is given by According to the above mass formulas, we find that it is impossible to extract the model parameters mQQ and vQQ

  • We find that the baryon masses obtained from the present improved chromomagnetic interaction (ICMI) model are consistent with the results from other theoretical approaches

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Summary

Introduction

Quantum chromodynamics (QCD) allows the existence of many fantastic hadrons, such as glueballs [1,2], hybrids [3,4], multiquark states (e.g., tetraquarks and pentaquarks) [5,6], and hadronic molecules [7,8]. The mass spectra and possible decay channels of the doubly charmed tetraquark states have been studied extensively by using the quark models [30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45], QCD sum rules [46,47,48,49,50,51,52], effective field theory [53,54,55,56], and lattice QCD [57,58,59,60,61,62,63,64]. We can construct all possible basis wave functions in the color and spin spaces for the tetraquark systems with given quantum numbers JP 1⁄4 0þ, 1þ, and 2þ.

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