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The terminal borylene complex 1 reacted with two
equivalents of supermesityl isonitrile (CNMes*) in non-
coordinating solvents (n-pentane, n-hexane, benzene, or
toluene) at room temperature to form a dark brown solution,
from which the complex [Cp(Mes*NC)(OC)Mn{C(O)B-
(tBu)(CNMes*)}] (2) precipitated out as a brown crystalline
solid quantitatively within minutes. Subsequent treatment of
2 with two equivalents of tris(pentafluorophenyl)borane,
which serves as a strong Lewis acid, led to quantitative
reformation of the terminal borylene 1. The reaction of 1 with
one equivalent of the isonitrile yielded a mixture of the
starting material 1 and the product 2 in a 1:1 ratio. Similarly,
addition of one equivalent of tris(pentafluorophenyl)borane
to a solution of 2 led to a 50% conversion of 2 into
1 (Scheme 2). No intermediate was detected in either the
forward or reverse reactions by 11B or 1H NMR spectroscopy.
These observations implied that both isonitrile ligands are
essential for formation and stabilization of complex 2.
optimized geometry are consistent with the experimentally
observed values. Therefore, the structural features of 2 will be
discussed based on calculated values.[17]
The energy-minimized geometry of 2 revealed two differ-
ently bonded bridging carbonyl ligands, which was also
reflected by experimental IR data and natural bond order
(NBO) analysis of model complexes of 2. The [C2O2]
carbonyl ligand (Figure 2) exhibits strong covalent interac-
tions with both Mn1 and B1 atoms, which involve the p*
antibonding orbital of CO, a dz2 orbital of the manganese
center, and the p orbital of the boron center (Figure 3). The
Figure 3. A) Depiction of the HOMOÀ8 of the model complex [Cp-
(PhNC)(OC)Mn{C(O)B(Me)(CNPh)}] (2H), showing the p-type bond-
ing interactions of the bridging carbonyl with the metal and boron
centers. B) Calculated Wiberg bond indexes and natural charges of the
model complex.
Scheme 2. Reversible coupling of the CO and B(tBu) ligands.
À
Single-crystal X-ray crystallography revealed the unusual
molecular structure of 2 as a cyclic complex with one bridging
and one semi-bridging carbonyl ligand between the Mn and B
Mn1 C2 separation of 1.938 ꢀ in 1 is noticeably longer than
those observed for other related bridging carbonyl-containing
derivatives (1.806–1.844 ꢀ).[18] The B1 C2 bond length is
À
atoms (Figure 2).[16] The coordination mode of M C(O) E
1.586 ꢀ, which lies in the range of a normal B C single
À
À
À
bond.[19] These parameters imply a somewhat stronger
interaction between the carbonyl [C2O2] and the boron
moiety than the manganese metal fragment, which was also
reflected by the Wiberg bond index (WBI) analysis. The
À
Mn1 C2 interaction has a WBI of 0.57, which is significantly
À
lower than that of B1 C2 (0.98). On the other hand, the
carbonyl [C1O1] has a quite different bonding situation. The
À
À
bond lengths of Mn1 C1 (1.784 ꢀ) and C1 O1 (1.168 ꢀ) are
not significantly different to those observed for a conventional
terminal carbonyl ligand. However, the WBI analysis
revealed a small but non-negligible bond order of 0.21
between C1 and B1. An interaction of similar strength was
found between Mn1 and B1, with a WBI of 0.24.
Figure 2. Molecular structure of 2. Ellipsoids are set at 50% proba-
bility. The ellipsoids of supermesityl groups are omitted for clarity.
Selected bond lengths [ꢂ] and angles [8] from B3LYP/Def2-SVP
calculations: Mn1–B1 2.297, Mn1–C1 1.784, Mn1–C2 1.938, Mn1–C12
1.847, B1–C1 2.229, B1–C2 1.586, B1–C8 1.662, B1–C12A 1.511; Mn1-
C1-O1 169.4, Mn1-C2-O2 137.9.
The bonding situation of the boron atom in 2 is rather
difficult to elucidate in terms of interactions with five
À
À
neighboring atoms. The covalent bonds B1 C2 and B1 C8
À
and the dative bond B1 C12A are more conventional, which
(M = transition metals, E = Group 13 element) was, to the
best of our knowledge, unknown prior to this work. We were
able to obtain crystals that contained benzene, toluene, or no
solvent molecules in the unit cell. However, all three
structures show the same type of disorder: an inversion
center in the middle of a molecule leads to overlap of
a {CpMnCO} moiety with {tBuBCO} that causes a problem
with deconvolution of atom positions, especially for the Mn/B
pair and both carbonyl groups. For this reason, computational
studies using density functional theory methods were per-
formed. The IR and NMR calculations of 2 based on
is also evident from the NBO analysis described above. The
third valence electron of boron must be pairing with one from
the metal center and forming a more delocalized interaction
with both Mn1 and C1. This more diffused, three-center–two-
electron bonding mode is also reflected by a remarkable
11B NMR chemical shift of À57 ppm (Table 1), which is
shifted by more than 200 ppm upfield from its precursor
borylene complex (1, 145 ppm).[18b] It lies considerablyfurther
upfield than those observed for not only the isonitrile
coordinated boron species, BR3(CNR’),[20] but indeed most
commonly observed tetracoordinate boron compounds
730
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2013, 52, 729 –733