Abstract

We study two- and three-gluon glueballs of C=+C=+ using the method of QCD sum rules. We systematically construct their interpolating currents, and find that all the spin-1 currents of C=+C=+ vanish. This suggests that the ``ground-state'' spin-1 glueballs of C=+C=+ do not exist within the relativistic framework. We calculate masses of the two-gluon glueballs with JPC=0±+/2±+J^{PC} = 0^{\pm+}/2^{\pm+} and the three-gluon glueballs with JPC=0±+/2±+J^{PC} = 0^{\pm+}/2^{\pm+}. We propose to search for the JPC=0−+/2−±/3±−J^{PC} = 0^{-+}/2^{-\pm}/3^{\pm-} three-gluon glueballs in their three-meson decay channels in future BESIII, GlueX, LHC, and PANDA experiments.

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