  The interaction of light with photonic resonators is determined by the
eigenmodes of the system. Modal theories based on quasinormal modes provide a
natural tool to calculate and understand light scattering by nanoresonators. We
show that, in the case of resonators made of absorbing dielectric materials,
eigenmodes with zero eigenfrequency (static modes) play a key role in the modal
formalism. The excitation of static modes builds a non-resonant contribution to
the modal expansion of the scattered field. This non-resonant term plays a
crucial physical role since it largely contributes to the off-resonance signal
to which resonances are added in amplitude, possibly leading to interference
phenomena and Fano resonances. By considering light scattering by a silicon
nanosphere, we quantify the impact of static modes. This study shows that the
importance of static modes is not just formal. Modal expansions without static
modes reconstruct an incorrect internal field and incorrect extinction and
absorption cross-sections. Static modes are of prime importance in an expansion
truncated to only a few modes.
