Abstract

We revisit the mixing mechanism for pesudscalar mesons and glueball which is introduced by the axial vector anomaly. We demonstrate that the physical mass of the pseudoscalar glueball does not favor to be lower than 1.8 GeV if all the parameters are reasonably constrained. This conclusion, on the one hand, can accommodate the pseudoscalar glueball mass calculated by Lattice QCD, and on the other hand, is consistent with the high-statistics analyses at BESIII that all the available measurements do not support the presence of two closely overlapping pseudoscalar states in any exclusive channel. Such a result is in agreement with the recent claim that the slightly shifted peak positions for two possible states $\eta(1405)$ and $\eta(1475)$ observed in different channels are actually originated from one single state with the triangle singularity interferences. By resolving this long-standing paradox, one should pay more attention to higher mass region for the purpose of searching for the pseudoscalar glueball candidate.

Highlights

  • The non-Abelian property of quantum chromodynamics (QCD) predicts the possible existence of glueball states as a peculiar manifestation of the strong interaction in the nonperturbative regime

  • One can check that the physical glueball mass MG keeps stable within the reasonable ranges of φQ and θ

  • Parameter Gg is fixed as jGgj 1⁄4 ð0.054 Æ 0.008Þ GeV3 from the quenched lattice QCD (LQCD) calculation

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Summary

INTRODUCTION

The non-Abelian property of quantum chromodynamics (QCD) predicts the possible existence of glueball states as a peculiar manifestation of the strong interaction in the nonperturbative regime. The observation of the significantly large isospin breaking effects in J=ψ →γηð1405=1475Þ→γ þ3π can be regarded as an indication of a special mechanism that causes the mysterious phenomena around 1.4–1.5 GeV for the isoscalar pseudoscalar meson spectrum [32].

THE MIXING FORMALISM
Constrain the parameters
Pseudoscalar glueball mass and its correlations with other parameters
Extracting topological susceptibilities for pseudoscalar mesons
Constraints on the charmonium state
SUMMARY
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