Abstract

We investigate a nonrelativistic model of tetraquarks, which are assumed to be compact and to consist of diquark-antidiquark pairs. We fit, for the first time, basically all currently known values for the measured masses of 45 mesons, including both charmed and bottom mesons, to the model and predict masses of tetraquarks as well as diquarks. In particular, we find masses of four axial-vector diquarks, i.e., $qc$, $cc$, $qb$, and $bb$, where $q = u,d$, and 24 ground-state tetraquarks, including both heavy-light tetraquarks ($qc\overline{qc}$ and $qb\overline{qb}$) and heavy tetraquarks ($cc\overline{cc}$ and $bb\overline{bb}$). In general, our results for the masses of $qb\overline{qb}$, $cc\overline{cc}$, and $bb\overline{bb}$ are largely comparable with other reported results, whereas our results for the masses of $qc\overline{qc}$ are slightly larger than what has been found earlier. Finally, we identify some of the obtained predictions for masses of tetraquarks with masses of experimental tetraquark candidates, and especially, we find that $\psi(4660)$, $Z_b(10610)$, and $Z_b(10650)$ could be described by the model.

Highlights

  • The concept of hadrons was introduced in 1962 by Okun [1] and developed into the quark model in 1964 independently by Gell-Mann [2] and Zweig [3,4], describing ordinary mesons and baryons in terms of quarks q and antiquarks q

  • The model of tetraquarks viewed as diquarkantidiquark systems is presented, and the method used to prescribe some tetraquark states quantitative masses is derived. This is preformed by firstly considering a quarkantiquark system and describing the Hamiltonian of that system with an unperturbed one-gluon exchange (OGE) potential and a perturbation term taking the spin of the system q1

  • Considering tetraquarks as bound states of axial-vector diquarks and antidiquarks, a simple model originally formulated for quarkonia has been adopted and used to calculate and predict the masses of different tetraquark states

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Summary

INTRODUCTION

The concept of hadrons was introduced in 1962 by Okun [1] and developed into the quark model in 1964 independently by Gell-Mann [2] and Zweig [3,4], describing ordinary mesons (qq ) and baryons (qqq) in terms of quarks q and antiquarks q. The ATLAS, CMS, and LHCb Collaborations were able to contribute with a massive amount of data on the electrically charge neutral Xð3872Þ, and its current mass is determined to be ð3871.69 Æ 0.17Þ MeV [7,13] It is the most studied exotic hadron, but its nature is still fairly unknown. Since the discovery of Xð3872Þ, many new exotic hadron candidates have been claimed to be observed with final states of a pair of heavy quarks and a pair of light antiquarks, which are labeled as X, Y, and Z states by experimental collaborations and collectively referred to as XYZ states [16]. With the masses of the diquarks determined, the initial stage of the model describing quark-antiquark systems is used to describe the diquark-antidiquark systems, which are interpreted as bound states of tetraquarks

Model procedure
MODEL AND FITTING PROCEDURE
Color structure
Fitting procedure
Data sets
Numerical fits and results
Diquarks
Tetraquarks
Motivation of parameters and comparison with other works
Discussion on results
Comparison with experimental results
SUMMARY AND CONCLUSIONS

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