arXiv · 2404.01564
The radiative decay of scalar glueball from lattice QCD
Abstract
We perform the first lattice QCD study on the radiative decay of the scalar glueball to the vector meson $\phi$ in the quenched approximation. The calculations are carried out on three gauge ensembles with different lattice spacings, which enable us to do the continuum extrapolation. We first revisit the radiative $J/\psi$ decay into the scalar glueball $G$ and obtain the partial decay width $\Gamma(J/\psi \to \gamma G)=0.578(86)~\text{keV}$ and the branching fraction $\text{Br}(J/\psi \to \gamma G) = 6.2(9)\times 10^{-3}$. We then extend the similar calculation to the process $G\to \gamma \phi$ and get the partial decay width $\Gamma(G \to \gamma \phi)= 0.074(47)~\text{keV}$, which implies that the combined branching fraction of $J/\psi\to\gamma G\to \gamma\gamma\phi$ is as small as $\mathcal{O}(10^{-9})$ such that this process is hardly detected by the BESIII experiment even with the large $J/\psi$ sample of $\mathcal{O}(10^{10})$. With the vector meson dominance model, the two-photon decay width of the scalar glueball is estimated to be $\Gamma(G\to\gamma\gamma)=0.53(46)~\text{eV}$, which results in a large stickiness $S(G)\sim \mathcal{O}(10^4)$ of the scalar glueball by assuming the stickiness of $f_2(1270)$ to be one.
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Jintao Zou, Long-Cheng Gui, Ying Chen, Jian Liang, Xiangyu Jiang, Wen Qin, Yi-Bo Yang. 2024-04-02. The radiative decay of scalar glueball from lattice QCD. https://doi.org/10.1007/s11433-024-2451-5
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