We investigate the problem of divergences appearing in the two-particle irreducible vertex functions of many-fermion systems with attractive on-site interactions. By means of dynamical meanfield theory calculations we determine the location of singularity lines in the phase diagram of the attractive Hubbard model at half-filling, where the local Bethe-Salpeter equations are non invertible. We find that divergences appear both in the magnetic and in the density scattering channels. The former affect a sector of suppressed fluctuations and are consistent with the mapping of the physical susceptibilities of the repulsive case. The appearance of singularities in the density channel demonstrate, instead, how vertex divergences can also plague the "dominant" scattering sectors associated with enhanced local susceptibilities, differently as observed for repulsive interactions. By introducing an insightful graphical representation of generalized susceptibilities and exploiting the underlying physical symmetries, we elucidate the relation between the two-particle vertices and the local response of the system, discussing algorithmic and physical implications of their singular behavior in the non-perturbative regime.