  We studied electronic excitations in NaV2O5 by Raman. Three main topics are
discussed. The first is related to a broad continuum of excitations found in
the 200-1500 cm-1 range and peaked around 680 cm-1. The resonant Raman profile
of this excitation, the polarization selection rules and the presence of its
overtone in resonance conditions allowed us to conclude that the origin of this
feature is magnetic. We proposed that it arises as a result of light coupling
to multi-spinon Raman excitations. Within this scenario we also argued for a
scenario explaining the puzzling temperature dependence of the magnetic
continuum in terms of an increasing role of next nearest neighbor frustration
and in the context of a strongly fluctuating low temperature phase. The second
topic is related to the observation of a folded S = 1 magnetic mode which
displayed very clear selection rules as a function of the magnetic field
orientation. We proposed that the coupling of the photon field to this
excitation takes place via the antisymmetric, Dzyaloshinskii-Moriya (DM),
interaction which, in a simple dimer model, can also explain the observed
selection rules: no splitting or shifts for magnetic fields parallel to the DM
vector and the observation of two (upward and downward) dispersing branches for
fields perpendicular to the DM vector. Thirdly, we discuss the nature of
several new resonances seen below T_c and focus on the possibilities that they
are either folded phonons or singlet bound states of two triplet excitations.
In particular we emphasized the existence of two modes at 66 and 105 cm-1, the
first one being degenerate with one of the spin gap modes.
