Abstract

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++0^{++} scalar states f0(1710)f_0(1710) and χc0(1P)χ_{c0}(1P), the 2++2^{++} states fJ(2220)f_J(2220) and χc2(2P)χ_{c2}(2P), the baryonic charmed state Ξc+(2645)Ξ_c^+(2645).

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