Inorganic Chemistry
Communication
results of X-ray diffraction analysis partially confirm our
speculation (Figure 1). That is, the carbene−boron bond
Figure 2. Results of DFT calculations on complexes BC and CC. Bond
lengths are shown in blue (Å), Wiberg bond indices in black, and natural
charges in red.
reveals a highly symmetrical η2-coordination of the B−C unit,
as indicated by almost identical Rh−B [2.027(8) Å] and Rh−C
[2.056(7) Å] bond lengths.4
Figure 1. Molecular structure of 3. Hydrogen atoms and ellipsoids of
ligands have been omitted for clarity. Ellipsoids drawn at the 50%
probability level. Selected bond lengths [Å] and angles [deg]: Rh−C2
2.126(2), Rh−C1 2.120(2), C1−C2 1.397(3), C1−B 1.438(3), B−C3
1.585(3), B−N1 1.533(3); C2−C1−B 146.0(2), Rh−C1−C2 71.0 (1),
Rh−C1−B 135.1(2).
In this contribution, we have reported the synthesis and full
characterization of a NHC-stabilized 1-boraallene coordinated to
rhodium by the reaction of (B,C-η2)-1-aza-2-borabutatriene
rhodium complex 1 with 2. The addition of the carbene to the
boron center induces a shift of the coordinated allene from BC
(BC) to a typical η2-CC (CC) mode. Interestingly, the released
BC double bond is in this case effectively stabilized by the
NHC and shows no subsequent intramolecular CH activation, as
observed in previous studies. DFT calculations on model species
CC and BC suggest that C−C coordination is thermodynami-
cally favored over B−C coordination by 25 kJ/mol.
formation is accompanied by a B−C to C−C coordination
1
mode change. Interestingly, while the H NMR signals of the
nitrogen-bound trimethylsilyl groups (δH 0.12) and of the
nitrogen-bound methyl groups (δH 3.63) appear as broad singlets
1
at ambient temperature, the H NMR spectrum shows clearly
two signals for N(SiMe3)2 (δH 0.38 and 0.00) and for NMe (δH
3.98 and 3.02) at −50 °C. This finding implies a certain degree of
rotational barrier about the B−N1 and B−C3 bonds. Never-
theless, the significantly elongated B−N1 bond of 1.533(3) Å
indicates the absence of substantial B−N π interaction. The B−
C3 bond length of 1.585(3) Å is comparable with that of NHC-
coordinated borabenzenes [1.596(2) Å] or 9-boraanthracenes
[1.607(4) Å].7 Hence, it can be anticipated that the rotational
barrier around the B−N1 and B−C3 bonds is due to steric
congestion between the bulky trimethylsilyl groups and the N-
bound methyl groups of the carbene unit. The B−C1 bond
length of 1.438(3) Å is comparable with those of noncoordinated
amino(methylene)boranes [e.g., 1.424(3) Å],2c thus indicating
the presence of a BC double bond. In contrast to the
previously reported thermally induced B−C to C−C coordina-
tion mode shift, the released BC double now displays no
reactivity toward the C−H bond of the coligand PCy3, thus
confirming the stabilizing effect of the carbene.
To gain further information about the observed B−C to C−C
coordination mode shift, DFT calculations on the model species
CC and BC were performed at the B3LYP level of theory (Figure
2). The calculated geometry of the model species CC, which is
derived from the title compound 3 by formal exchange of the
PCy3 ligand by a PMe3 group, is in excellent agreement with the
results of the X-ray structure analysis. Not surprisingly, the
calculations predict that the B−C coordination mode is 25 kJ/
mol higher in energy, thus suggesting that the model species CC
represents the thermodynamically favored product. Further-
more, the central B−C bond in the hypothetical isomer BC
coordinates in a highly distorted η2−π fashion, as indicated by the
calculated geometry. That is, the Rh−B bond (2.381 Å) is
significantly longer than the endocyclic Rh−C bond (2.053 Å).
In contrast, the crystal structure of the aforementioned (carbene-
free) (B,C-η2)-1-aza-2-borabutatriene rhodium complex 1
ASSOCIATED CONTENT
* Supporting Information
Experimental section, X-ray crystallographic details including a
CIF file, and computational details. This material is available free
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S
AUTHOR INFORMATION
Corresponding Author
Notes
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The authors declare no competing financial interest.
ACKNOWLEDGMENTS
Financial support by the European Research Council (Advanced
Investigator Grant to H.B.) is gratefully acknowledged.
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