The X-ray crystal structure of
[Li−C⋮C−SiMe2−C6H4−OMe]6
(14)6 features nearly symmetric
π-interactions between the lithium ions and the acetylide anions
(Li1−Cβ = 2.353(9) Å,
Li1−Cα = 2.292(9) Å).
These π-contacts are facilitated by the chelating
o-anisyl methoxy groups
(Li1−Cα−Cβ =
77.6(4)°, Li1−O1 =
2.169(9)
Å). The Li−Cα distances in the
(LiCα)6 core of (14)6
differ significantly (Li1α−Cα =
2.132(9) Å, Li1b−Cα =
2.205(11) Å). This Li−Cα distance
differentiation is unique in organolithium hexamers, and is due to
Li(C⋮C−R)
“side-on-π” and “end-on-σ” contacts, as is shown
computationally in H−C⋮C−Li(LiH)2
(20). A second X-ray
crystal structure,
[Li−O−CMe2−C⋮C−H]6
(22)6, reveals electrostatic π-interactions
between the lithiums in the
(LiO)6 core and the nonmetalated acetylene groups
(Li1−C2 = 2.443(5) Å,
Li1−C3 = 2.749(6) Å). These
Li−C
π-contacts shorten upon acetylene lithiation, as is shown
computationally in Li−O−CH2−C⋮C−(H/Li)
(24-H/Li).
Additional computations reveal that the π-interactions in
(HC⋮C)M2H (26-Li-Cs) complexes (modelling
oligo- and
polymeric M−C⋮C−R) are weak (only 0.7 kcal/mol for Li), but
substantial in M+(H−C⋮C−H)
(27-Li-Cs) species
(20.2 kcal/mol for Li+). In 26-Li-Cs, the
π-contacts increase the C⋮C bond lengths slightly (0.005 Å for Li)
and
lower the C⋮C stretching frequencies (33 cm-1 for Li),
they polarize charge density from Cα toward
Cβ and hence
result in counterion-induced charge delocalizations. The degrees
of π-interactions both in (26-Li-Cs) and in
(27-Li-Cs) decrease with increasing size of the alkali
cations.