  According to lattice simulations and other theoretical approaches, the scalar
glueball is the lightest state in the Yang-Mills sector of QCD. Since within
this sector the scalar glueball is stable, the scattering between two glueballs
is a well-defined process. Moreover, a glueball-glueball bound state, called
glueballonium, might exist if the attraction turns out to be large enough. In
this work, we concentrate on the formation of the glueballonium in the context
of the dilaton potential. In particular, we investigate the parameter values
for which such a glueballonium emerges.
