Abstract

We apply the method of QCD sum rules to study the $s q \bar s \bar q$ tetraquark states with the exotic quantum number $J^{PC} = 3^{-+}$, and extract mass of the lowest-lying state to be $2.33^{+0.19}_{-0.16}$ GeV. To construct the relevant tetraquark currents we need to explicitly add the covariant derivative operator. Our systematical analysis on their relevant interpolating currents indicates that: a) this state well decays into the $P$-wave $\rho\phi/\omega\phi$ channel but not into the $\rho f_2(1525)/\omega f_2(1525)/\phi f_2(1270)$ channels, and b) it well decays into the $K^*(892) \bar K_2^*(1430)$ channel but not into the $P$-wave $K^*(892) \bar K^*(892)$ channel.

Highlights

  • We apply the method of QCD sum rules to study the sqsqtetraquark states with the exotic quantum number JPC 1⁄4 3−þ, and extract mass of the lowest-lying state to be 2.33−þ00

  • There have been many candidates of exotic hadrons observed in particle experiments, which cannot be well explained in the traditional quark model [1,2,3,4,5,6,7,8,9,10]

  • There exist some “exotic” quantum numbers that traditional hadrons cannot have, such as the spin-parity quantum numbers JPC 1⁄4 0−−, 0þ−, 1−þ, 2þ−, 3−þ, etc. These exotic quantum numbers are of particular interest, because the hadrons with such quantum numbers cannot be explained as traditional hadrons any more

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Summary

INTRODUCTION

There have been many candidates of exotic hadrons observed in particle experiments, which cannot be well explained in the traditional quark model [1,2,3,4,5,6,7,8,9,10]. The same QCD sum rule method was applied to extensively study light tetraquark states of JPC 1⁄4 0−− in Refs. We shall investigate the light qsqs ̄ (q 1⁄4 up=down and s 1⁄4 strange) tetraquark states with such a quantum number. They may exist in the energy region around 2.0 GeV. In this paper we shall investigate the qsqs ̄ tetraquark state with the exotic quantum number JPC 1⁄4 3−þ using the method of QCD sum rules. In the present study we shall improve it by explicitly adding the covariant derivative operator in order to construct the qsqs ̄ tetraquark currents of JPC 1⁄4 3−þ.

INTERPOLATING CURRENTS
CCCCCCCCCCA:
QCD SUM RULE ANALYSIS
NUMERICAL ANALYSES
SUMMARY AND DISCUSSIONS
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