  Strong decays of $X\left( 3915\right) $ are analyzed from two quark model
descriptions of $X\left( 3915\right) $, a conventional one in terms of the
Cornell potential and an unconventional one from a Generalized Screened
potential. We conclude that the experimental suppression of the OZI allowed
decay $X\left( 3915\right) \rightarrow D\overline{D}$ might be explained in
both cases as due to the momentum dependence of the decay amplitude. However,
the experimental significance of the OZI forbidden decay $X\left( 3915\right)
\rightarrow\omega J/\psi$ could favor an unconventional description.
