Abstract

Matrix elements of the form are calculated using the lattice QCD Monte Carlo method. Here, G>|G> is a glueball state with quantum numbers 0++ 0^{++}, 2++ 2^{++}, 0+ 0^{-+} and GG is the gluon field strength operator. The matrix elements are obtained from the hybrid correlation functions of the fuzzy and plaquette operators performed on the 12412^{4} and 14414^{4} lattices at β=5.9\beta = 5.9 and 5.965.96 respectively. These matrix elements are compared with those from the QCD sum rules and the tensor meson dominance model. They are the non-perturbative matrix elements needed in the calculation of the partial widths of J/ΨJ/\Psi radiative decays into glueballs.Comment: 12 pages, UK/92-0

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    Last time updated on 01/04/2019