  Chiral symmetry restoration in high-lying hadron spectra implies that hadrons
which belong to different irreducible representations of the parity-chiral
group cannot mix. This explains why the $f_0(2102 \pm 13)$, which was suggested
to be a glueball, and hence must belong to the scalar (0,0) representation of
the chiral group, cannot mix with the neighbouring $f_0(2040 \pm 38)$, which
was interpreted as a $ n\bar n$ state, and that belongs to the $(1/2,1/2)$
representation of the chiral group. If confirmed, then we have an access to a
"true" glueball of QCD.
