Abstract

In pure-glue QCD, gluon-gluon scattering in the JPC=0−+J^{PC}=0^{-+} channel is described by a very simple equation, especially if one considers just the leading contribution to the scattering kernel. Of all components in this kernel, only the three-gluon vertex, VμνρV_{μνρ}, is poorly constrained by contemporary analyses; hence, calculations of 0−+0^{-+} glueball properties serve as a clear window onto the character and form of VμνρV_{μνρ}. This is important given that many modern calculations of VμνρV_{μνρ} predict the appearance of an infrared suppression in the scalar function which comes to modulate the bare vertex after the nonperturbative resummation of interactions. Such behaviour is a peculiar prediction; but we find that such suppression is essential if one is to achieve agreement with lattice-QCD predictions for the 0−+0^{-+} glueball mass. It is likely, therefore, that this novel feature of VμνρV_{μνρ} is real and has observable implications for the spectrum, decays and interactions of all QCD bound-states.

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