Abstract

The mass components of charmoniumlike states are investigated through the decomposition of QCD energy-momentum tensor (EMT) on lattice. The quark mass contribution $\langle H_m\rangle$ and the momentum fraction $\langle x\rangle$ of valence charm quark and antiquark are calculated for conventional $1S,1P,1D$ charmonia and the exotic $1^{-+}$ charmoniumlike state, based on the $N_f=2+1$ gauge configurations generated by the RBC/UKQCD collaboration. It is found that $\langle H_m\rangle$ is close to each other and around 2.0 to 2.2 GeV for these states, which implies that the mass splittings among these states come almost from the gluon contribution of QCD trace anomaly. The $\langle x\rangle$ of the $1^{-+}$ state is only around 0.55, while that in conventional charmonia is around 0.7 to 0.8. This difference manifests that the proportion of light quarks and gluons in the $1^{-+}$ charmoniumlike state is significantly larger than conventional states.

Highlights

  • Based on the quantum chromodynamics (QCD) the gluon is massless and the intermedia of the strong interaction

  • The quark mass contribution hHmi and the momentum fraction hxi of valence charm quark and antiquark are calculated for conventional 1S, 1P, 1D charmonia and the exotic 1−þ charmoniumlike state, based on the Nf 1⁄4 2 þ 1 gauge configurations generated by the RBC/ UKQCD collaboration

  • We investigated mass decomposition of conventional 1S, 1P, 1D charmonia and exotic 1−þ charmoniumlike state

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Summary

INTRODUCTION

Based on the quantum chromodynamics (QCD) the gluon is massless and the intermedia of the strong interaction It is well-know that gluons bind light quarks into massive hadrons, there is a question that how much gluons contribute to the total mass of a hadron. One must establish the connection of the lattice states in this channel to the possible physical states in the Lüscher formalism [9,10] by studying the related mesonmeson scatterings. This requires certainly sophisticated numerical techniques to tackle the annihilation diagrams of light quarks and to derive precise energy levels.

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