Communication
calculated equilibrium geometries of the doublet
state (2m) and the quartet state (2m) of CoL2 sug-
gest that the doublet state 2m resembles more
closely to the crystal structure of 2. Note that the
quartet state 2m’ is 16.9 kcalmolꢀ1 higher in energy
than the doublet state 2m (Figure S3 in the Sup-
porting Information). Thus, the geometrical data and
relative energy indicate the doublet 2m as the
ground state. The Co center in 2m exists in a bent
geometry with the bending angle of 168.28. The di-
hedral angle between the planes of the two cAAC: ligands in
2m (78.88) indicates that the two cAAC: ligands are almost
perpendicular to each other. The CoꢀCcAAC bond length is
slightly longer, and the CcAACꢀN bond lengths are slightly short-
er in 2m than the corresponding bond lengths in the previ-
ously reported (Me2ꢀcAAC:)2Co2.[11] Note also that the CcAACꢀN
bond length is significantly longer than the CcAACꢀN bond
length in free cAAC:, which signifies Co!CꢀN p*-back dona-
tion. Hence, these geometrical data suggest that 2m can be
considered as a bent 2-metallaallene.[12]
Scheme 1. Syntheses of (Me2-cAAC:)2Co0 (2) from (cAAC:)2CoICl (1).
mamide solution of 1, containing 0.1m nBu4NPF6 as electrolyte,
showed a one-electron quasi-reversible reduction at E1/2
ꢀ0.57 V versus (Cp*2Fe)/(Cp*2Fe)+ indicating the possible for-
mation of 2 (Figure 1). Indeed, compound 2 was chemically
synthesized from 1 (Scheme 1).
=
The 1:1 molar mixture of (Me2-cAAC:)2CoICl (1) and KC8 react-
ed in THF to give a dark blue solution, which was filtered
(Scheme 1). This solution was slowly concentrated under
vacuum to form dark shiny needles of (Me2-cAAC:)2Co0 (2),
which are separated by filtration and dried in vacuum, giving
98% yield. The volume of the solvent should be maintained to
carry out a cleaner reaction to obtain such high yields (see the
Supporting Information). However, it is important to mention
that the yield of 2 dropped upon decreasing the volume of
the solvent. Compound 2 can also be synthesized within fif-
teen minutes by the reduction of precursor 1 at room temper-
ature in a similar yield when 2.2 equivalents of LiNiPr2 (LDA)
were employed as a reducing agent, instead of one equivalent
of KC8 (see the Supporting Information). The detailed synthesis,
purification, and characterization of compound 2 are given in
the Supporting Information. Compound 2 is stable in an inert
atmosphere and decomposes above 1348C. It produces a blue
color when dissolved in organic solvents, such as THF, toluene,
The natural bond orbital (NBO) charge analysis revealed that
the Co center in 2m is positively charged (0.122 e), and hence
the CcAAC!Co s donation can be considered as being weaker
!
than the CcAAC Co p-back donation.[10] This is reflected in the
smaller Wiberg bond index of the CꢀN bond (1.31) compared
with the corresponding value in free cAAC: (1.50). On the one
hand, the NBO spin density in 2m showed significant accumu-
lation of a spin on the Co atom (1.526). On the other hand,
the b-spin density is delocalized over the cAAC: ligand with
major coefficient on the carbene C and the N atoms (0.253;
Figure 3a). This results in one unpaired electron of 2m. The
Mulliken charge and spin density analysis also give similar re-
sults (Table S3 in the Supporting Information). Such accumula-
tion of excess a-spin density at the metal center and delocali-
zation of the b-spin over the cAAC: ligands was also observed
for the recently reported (cAAC:)2Mn complex.[13] The bonding
1
and benzene. H NMR spectrum of 2 showed broad resonances
ranging from d=ꢀ2.5 to 10 ppm indicating the paramagnet-
ic[7–9] nature of the solution, as was expected. Compound 2
can be further characterized by MS (EI) spectrometry (m/z
(100%): 629.4; see the Supporting Information). The reaction
energy for the formation of 2 from 1 was calculated (at the
M06/def2-TZVPP//BP86/def2-SVP level of theory) to be exo-
thermic by ꢀ17.2 kcalmolꢀ1 (KC8 as a reducing agent), which
also indicates the feasibility of the reaction (Scheme 1).
¯
Compound 2 crystallizes in the triclinic space group P1. The
central cobalt atom is bound to two carbene carbon atoms
adopting a two-coordinate bent geometry (Figure 2). The C-
Co-C bond angle is 170.12(8)8, which is far wider when com-
pared with that of precursor 1 (122.33(10)8). The CoꢀCcAAC and
NꢀCcAAC bond lengths of 2 are 1.871(2)/1.877(2) and 1.343(2)/
1.349(2) ꢀ, respectively, which are close to the values of
1.920(2)/1.932(2) and 1.335(3)/1.333(3) found in 1.[6] The slight
shortening of the CoꢀCcAAC bond lengths and increasing of
CcAACꢀN bond lengths might be due to the Co!CcAAC p-back
donation.
Figure 2. Molecular structure of compound 2. Hydrogen atoms are omitted
for clarity. Selected experimental [calculated ones at the BP86/def2-SVP level
for the ground state] bond lengths [ꢀ] and angles [8] from single-crystal X-
ray diffraction: Co1ꢀC1 1.871(2) [1.883], Co1ꢀC21 1.877(2) [1.884], C1ꢀN1
1.343(2) [1.362], C21ꢀN2 1.349(2) [1.362]; C1-Co1-C21 170.12(8) [168.2], C2-
C1-N1 106.67(16) [106.3], N2-C21-C22 106.81(15)[ 106.3], C2-C1-Co1
122.51(14) [121.9], N1-C1-Co1 130.69(13) [131.4].
We have performed theoretical calculations at the M06/def2-
TZVPP//BP86/def2-SVP level of theory for the different spin
states of the two-coordinate cobalt model compound CoL2
(L=Me2-cAAC:) (2) using Gaussian 09 program package.[10] The
Chem. Eur. J. 2014, 20, 11646 – 11649
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