Communications
Figure 1. Crystal structure of 2. Ellipsoids are set at the 50% proba-
bility level. Hydrogen atoms are omitted for clarity. Selected bond
lengths [ꢂ] and angles [8]: B–C5 1.541(2), B–C1 1.535(2), B–C4
1.541(2), C1–C2 1.431(1), C2–C3 1.446(1), C3–C4 1.41(1), C5–N1
1.371(1), C5–N2 1.374(1); C1-B-C5 128.55(10), C1-B-C4 104.95(9), C4-
B-C5 125.79(10), B-C1-C2 107.21(9), C1-C2-C3 109.57(9), C2-C3-C4
111.36(9), C3-C4-B 106.86(9).
Figure 2. Depiction of the HOMO of 2’.
interaction. This electronic situation of 2 is somewhat inverse
to that of boryl anions of type A, in which the lone-pair
electrons occupy an exocyclic sp2 orbital, while the pz orbital
of boron is stabilized by p bonding to the adjacent nitrogen
atoms.[2d,16] In compound 2, however, the electron density
preferentially resides in the pz orbital of the boron atom,
while the NHC donates its lone pair into the equatorial sp2
orbital. The NHC ligand serves not only as a strong s donor
but also as a p acceptor in delocalizing the electrons from the
boron atom.
For probing the nucleophilicity of the boron atom,
compound 2 was treated with an excess of MeI in Et2O at
ambient temperature. After workup, the NHC-coordinated 1-
methyl-2,3,4,5-tetraphenylborole (3) was isolated as a color-
less solid in 71% yield. The resonance of 3 in the 11B NMR
spectrum detected at d = À10.8 ppm is significantly shifted
upfield compared to that detected for 2, in agreement with the
¯
dimer in the space group P1 (Figure 1; only one half is
displayed; the dimer is depicted in Figure S1). Within the
dimer unit, the potassium cation resides above one of the
borole rings and coordinates to the phenyl substituent at the
C2 atom of the other borole molecule through an intermo-
lecular cation–p interaction (Figure S1 in the Supporting
Information). The borole ring is essentially planar with an
average displacement of the ring atoms above the C4B plane
of 0.0085 ꢀ. The boron atom adopts the trigonal-planar
geometry, as indicated by the sum of angles of 359.38. In
À
comparison with the neutral boroles, the intraannular C C
bond-length alternation within the C4B ring is significantly
decreased.[13] The B C1 and B C4 bonds are also shorter
than those observed in neutral boroles.[12b] In fact, the
structural features of 2 within the borole ring resemble
those of borole dianions, thus emphasizing the aromatic
À
À
1
formation of a tetracoordinate boron center. The H reso-
character of the C4B ring in 2.[12b] The B C5 bond of
nance of the methyl (B Me) group at d = À0.4 ppm is also
À
À
1.5406(15) ꢀ is also significantly shorter than that of the
NHC-coordinated borabenzenes (1.596(2) ꢀ)[14] or 9-boraan-
thracenes (1.607(4) ꢀ).[9d] This finding together with a
relatively small dihedral angle of 36.38 between the carbene
ligand and borole moiety suggests non-negligible p bonding
between the boron atom and the exocyclic carbene ligand.[15]
To better understand the electronic structure of 2,
computations of the model complex 2’ were performed with
DFT methods at the B3LYP/6-31g* level of theory. Complex
2’, in which the mesityl groups are replaced by 2,6-dimethyl-
phenyl groups, was optimized as a monomer in the absence of
the potassium ion coordination. The energy-optimized geom-
etry of 2’ is in good agreement with that determined
experimentally, thus indicating that the critical bonding
features are captured in the model complex. Examination of
the electron density distribution of the HOMO of 2’ indeed
reveals a p-like bonding orbital between the boron atom and
carbene carbon center with significant contribution from
boron atom (14.6%), suggesting the presence of a p-
nucleophilic boron atom (Figure 2). This finding also implies
the existence of a considerable p-back-bonding contribution
from boron to carbon to the overall borole–carbene bonding
shifted upfield with respect to those of the methyl protons of
the mesityl groups. As a result of the quadrupolar coupling
with the boron nuclei, the signal of the boron-bound methyl
group in the 13C NMR spectrum detected at d = 8.2 ppm is
very weak and was only identified by HMQC methods.
Single crystals suitable for X-ray analysis were obtained
from slow evaporation of a Et2O/n-hexane solution of 3 at
room temperature. Compound 3 crystallizes in the monoclinic
P21/c space group and displays two independent molecules in
the asymmetric unit (Figure 3). These two independent
molecules feature similar structural parameters and are
arbitrarily denoted as molecule I and molecule II. The
propeller-like arrangement of the phenyl groups with average
dihedral angles of 53.28 (I) and 56.88 (II) represents the
common structural feature of tetraphenyl-substituted boroles.
The boron atom adopts a distorted tetrahedral environment,
À
and all B C bond lengths fall within the expected range for
the corresponding single bonds. The significant elongation of
À
À
the B C1 [1.649(2) ꢀ (I); 1.650(2) ꢀ (II)] and B C4 bonds
[1.648(2) ꢀ (I); 1.650(2) ꢀ (II)] compared to those observed
in 2 indicates the loss of p-electron delocalization over the
C4B ring mediated by the pz orbital of the boron atom.
ꢀ 2010 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2010, 49, 2041 –2044