  In the present work a consistent kinematic-based framework for glueball
states is proposed. It relates the glueball, the Pomeron, QCD lattice
calculations, the $0^{++}$ scalar states $f_0(1710)$ and $\chi_{c0}(1P)$, the
$2^{++}$ states $f_J(2220)$ and $\chi_{c2}(2P)$, the baryonic charmed state
$\Xi_c^+(2645)$.
