Why X(3872) is not a molecule
We discuss the scenario where the X(3872) resonance is the c c-bar = χ{sub c1}(2P) charmonium which “sits on” the D*{sup 0} D-bar {sup 0} threshold. We explain the shift of the mass of the X(3872) resonance with respect to the prediction of a potential model for the mass of the χ{sub c1}(2P) charmonium by the contribution of the virtual D* D-bar + c.c. intermediate states into the self energy of the X(3872) resonance. This allows us to estimate the coupling constant of the X(3872) resonance with the D*{sup 0} D-bar {sup 0} channel, the branching ratio of the X(3872) → D*{sup 0} D-bar {sup 0} + c.c. decay, and the branching ratio of the X(3872) decay into all non-D*{sup 0} D-bar {sup 0} + c.c. states. We predict a significant number of unknown decays of X(3872) via two gluon: X(3872) → gluongluon → hadrons. We suggest a physically clear program of experimental researches for verification of our assumption.