The structural, rotational, and vibrational properties of C
n
- clusters (n = 3−13) have been investigated by
means of density functional theory (DFT/B3LYP) and, whenever possible, coupled cluster (CC) theory along
with the aug-cc-pVDZ basis set. These properties are compared with those of their neutral counterparts and
of the corresponding cations. The linear and merely cumulenic chains undergo a substantial increase of the
bond-length alternation and an increase of size upon adiabatic electron attachment. In addition, most chains
(C5, C7, C8, C9, and C10) become slightly bent in their anionic form because of Renner−Teller effects. The
structural outcomes of such processes on carbon rings are far more varied and can be rationalized solely
through a topological analysis of the frontier orbitals. Both for the linear and cyclic species, IR spectra and
rotational moments provide specific markers of these complex structural variations. Closed anionic clusters
such as C5
-, C9
-, and C13
- are even-twisted cumulenic rings. The highest occupied levels of these rings
relate to orbitals with a particularly exquisite bonding pattern, which explains, among other effects, significant
departures from planarity. It has been noticed that d diffuse functions are essential for a sound description of
the Renner−Teller distortions of C
n
- chains and of the nonplanar nature of the C13
- ring. The linear anionic
chains exhibit a much stronger IR activity, as well as a systematically greater propensity to bind an extra
electron, than the cyclic isomers. Among the rings, the adiabatic electron affinities (AEAs) of the C9 and C13
species are strikingly high, whereas the lowest value of AEA coincides with the cumulenic C10 species. For
the anionic chains and the larger rings, the most intense IR absorption lines have vibrational frequencies
ranging from 1600 to 2200 cm-1.