Abstract

We have studied the masse spectra for the $cc\overline{b}\overline{b}$ and $bb\overline{c}\overline{c}$ tetraquark states with quantum numbers ${J}^{P}={0}^{\ifmmode\pm\else\textpm\fi{}},{1}^{\ifmmode\pm\else\textpm\fi{}}$, and ${2}^{+}$. We systematically construct the interpolating currents with various spin-parity quantum numbers and calculate their two-point correlation functions in the framework of QCD moment sum rule method. Our calculations show that the masses are about 12.3--12.4 GeV for the positive parity $cc\overline{b}\overline{b}$ tetraquark ground states with ${J}^{P}={0}^{+},{1}^{+},{2}^{+}$, while 12.8--13.1 GeV for the negative parity channels with ${J}^{P}={0}^{\ensuremath{-}},{1}^{\ensuremath{-}}$. The mass predictions for the positive parity $cc\overline{b}\overline{b}$ ground states are lower than the ${B}_{c}{B}_{c}$ threshold, implying that these tetraquarks can only decay via weak interaction and thus are expected to be stable and narrow.

Highlights

  • The existence of multiquarks was first proposed by Murray Gell-Mann and George Zweig at the birth of the quark model in 1964 [1,2], in which hadrons were classified as qqmesons and qqq baryons

  • Our calculations show that the masses are about 12.3–12.4 GeV for the positive parity ccbbtetraquark ground states with JP 1⁄4 0þ; 1þ; 2þ, while 12.8–13.1 GeV for the negative parity channels with JP 1⁄4 0−; 1−

  • The mass predictions for the positive parity ccbbground states are lower than the BcBc threshold, implying that these tetraquarks can only decay via weak interaction and are expected to be stable and narrow

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Summary

INTRODUCTION

The existence of multiquarks (qqqq ̄ tetraquark, qqqqqpentaquark, etc.) was first proposed by Murray Gell-Mann and George Zweig at the birth of the quark model in 1964 [1,2], in which hadrons were classified as qqmesons and qqq baryons. In 2017, the CMS Collaboration reported their measurement of an exotic excess around 18.4 GeV in the four lepton channel with a global significance of 3.6σ [12], which had inspired lots of theoretical studies on the bbbb ̄ four-bottom tetraquark states [13,14,15,16,17,18,19,20,21,22] Such an exotic structure was not confirmed by the later experiments [23,24]. [14], the ground state, energy of the ccbb ̄ tetraquarks were calculated in a nonrelativistic effective field theory and in a diquark model They gave an upper limit on mass of ccbb ̄ tetraquark as 12.58 GeV below the 2Bc threshold, indicating the possibility of stable ccbb ̄ tetraquark against strong decays.

INTERPOLATING TETRAQUARK CURRENTS
QCD SUM RULES
NUMERICAL ANALYSIS
CONCLUSION AND DISCUSSION
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