Abstract
The radiative decay of \$J/\psi\$ into a pure gauge tensor glueball is studied
in the quenched lattice QCD formalism. With two anisotropic lattices, the
mutlipole amplitudes E\_1(0), M\_2(0) and E\_3(0) are obtained to be 0.114(12)GeV,
-0.011(5)GeV and 0.023(8)GeV, respectively. Thus the partial decay width
\$\Gamma(J/\psiG\_2^++)\$ is estimated to be 0.99(22)keV
which corresponds to a large branch ratio 1.1(2)x10^-2. The phenomenological
implication of this result is also discussed.
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