  The ee$\in$MC generator package is extended to include $e^{+}e^{-} \to
Hadrons (n\gamma)$ events where the photons can be generated in either the
initial-state or final-state production. In particular, the $e^{+}e^{-} \to
\pi^{+}\pi^{-} (n\gamma)$, $e^{+}e^{-} \to \Upsilon(4s) (m\gamma) \to
B^{+}B^{-} (n\gamma)$ and $e^{+}e^{-} \to \Upsilon(4s) (m\gamma) \to
B^{0}\bar{B}^{-} (n\gamma)$ decay channels have been implemented in the
generator. The B-mesons are not decayed in ee$\in$MC, but are left for other
generators that specialized in B-mesons. Both the initial-state-radiation and
final-state-radiation are simulated using the Yennie-Frautschi-Suura
Exponentiation procedure \cite{Yennie:1961}, where several effective models are
implemented to investigate the assumption of the radiative structure of the
final-state vertex. The impact of these radiative models on the $e^{+}e^{-} \to
\Upsilon(4s) (m\gamma) \to B^{+}B^{-} (n\gamma)$ and $e^{+}e^{-} \to
\Upsilon(4s) (m\gamma) \to B^{0}\bar{B}^{-} (n\gamma)$ processes, excludes some
models, particularly, in regards to the Coulomb potential. This has an
important impact for meson and baryon systems near threshold.
