  When an unstable ordinary quark-antiquark state couples strongly to other
low-mass mesons (such as pions, kaons, $D$-mesons, etc.), the quantum
fluctuations generated by the decay products dress the bare `seed' $\bar{q}q$
state and modify its spectral functions. The state is associated to a pole on
the complex plane. When the coupling to the decay products is sufficiently
large, a remarkable and interesting phenomenon takes place: dynamically
generated companion states (or poles) might emerge. Some resonances listed in
the PDG , such as the $a_{0}(980),$ the $K_{0}^{\ast}(700),$ and the $X(3872),$
can be well understood by this mechanism, that we briefly review in these
proceedings. On the other hand, we show that the $Y(4008)$ and $Y(4260)$ are
not independent resonances (or poles), but manifestations of $\psi(4040)$ and
$\psi(4160),$ respectively.
