2.2 ppm, whereas the Ru–C resonance appears shielded at
24.8 ppm (JC–H = 141 Hz) in the 13C NMR spectrum. One
31P{1H} NMR singlet is observed at 56.9 ppm at all accessible
temperatures.17
Complex 5 is also obtained quantitatively upon dihydrogen loss
from solutions of 3. Moreover, even under a dihydrogen
atmosphere, THF, benzene or toluene solutions of 3 are not
stable over a period of days and 5 is formed presumably via the
mixed complex RuH{g2-H–SiMe2CH2(o-C6H4)PPh2}{g2-H–
SiMe2CH(o-C6H4)PPh2} (6) as detected spectroscopically.
Independently, 6 can also be obtained as the major product from
the reaction of 4 with 2 equiv of 2 under 3 bar of dihydrogen for
two hours. The main NMR features of complex 6 are two 29Si
NMR signals at d = 11 ppm and at d = 213 ppm for the non-
metallated and the carbometallated ligands respectively, and two
31P{1H} NMR doublets (d 56.5 and 42.7 ppm, 2JP–P 21 Hz). The
three hydride resonances appear as a broad signal at d = 26.0 ppm
(JSi–H = 76 Hz), a pseudo-triplet at 28.0 ppm (JP–H = 21 and
27 Hz) and a doublet of doublets at 29.4 ppm (JP–H = 24 Hz and
54 Hz). The JSi–H value is in agreement with the presence of at least
one agostic Si–H bond and a SISHA interaction.5f The proposed
structure is consistent with the ground-state structure of 6
computed at the DFT/B3PW91 level (see ESI{).
Agostic C–H interactions preluding C–H activation are well
known,4,18 and Berry et al. have described tandem b-C–H
activation/Si–H elimination reactions.6 We show here that the
bis(agostic) Si–H complex 3, displaying rare high order e-agostic
Si–H interactions (to the best of our knowledge no precedent
higher than d-agostic is known) leads finally to 5, with two
b-agostic interactions as a result of C–H activations. The increased
acidity of the methylene groups of the ligand in complex 3 coupled
with the presence of agostic Si–H bonds, which can easily
decoordinate, induce a stepwise H2-loss process resulting ulti-
mately in the formation of the stable bis(carbometallated) complex
5. Whilst C–H activation occurring a to a heteroatom could be
expected,4 it is worth noting that in our system such a reaction
proceeds with final preservation of the agostic Si–H bonds in 5 and
6. A facile dissociation–recoordination pathway could end in the
formation of the carbometallated species whilst reforming the
agostic Si–H bonds in the final stable products. Although no
conclusive mechanistic evidence could be found, the agostic Si–H
interactions favour in some way the C–H activation process.
This work was supported by CONACYT grant 43540 and
CNRS/CONACYT grant 16873. We thank the CINES
(Montpellier, France) for a generous allocation of computer time
and Miss Hanit Trevin˜o for laboratory assistance.
Fig. 1 X-Ray structure of 5 (top) and computed DFT/B3PW91 structure
of 5b (bottom) (non-relevant H atoms omitted for clarity). Ellipsoids in 5
are shown at the 50% probability level. Selected bond lengths (s) and
angles (u), with the DFT data in parenthesis for comparison: Ru–Si(1)
2.4587(13) (2.454), Ru–Si2 2.4367(13) (2.454), Ru–C19 2.263(4) (2.241),
Ru–C24 2.244(4) (2.241), Ru–H100 1.71(4) (1.709), Ru–H101 1.68(4)
(1.709), Si2–H100 1.76(4) (1.709), Si1–H101 1.65(3) (1.709), Si1–Ru–Si2
120.01(5) (121.02), P1–Ru–P2 107.10(4) (102.50), H100–Ru–H101
175.1(18) (178.94), Ru–H101–Si1 95.2(19) (91.80), Ru–H100–Si2
89.4(18) (91.80).
isomers (see ESI{) with the phosphorus in a trans (3a) or cis (3b)
disposition were optimized. 3a being the highest in energy
(+33.6 kJ mol21).
More interestingly, when the addition of 2 was performed
on Ru(COD)(COT) (4), the new species Ru{g2-H–SiMe2CH(o-
C6H4)PPh2}2 (5) was detected as the sole product by 1H and
31P{1H} NMR spectroscopy, and isolated in 92% yield (Scheme 1).
Its formulation as a bis(cyclometallated) species, resulting from
C–H activation of the methylene groups of the starting ligand 2,
was ascertained from NMR, X-ray{ and consistent with DFT
data. The molecular structure of 5 is shown in Fig. 1. The
geometry around the ruthenium centre is a bicapped pseudo-
octahedron with Si atoms capping and a cis disposition of the
other heavy atoms. Two modified phosphinobenzylsilane ligands
coordinate to the metal each through a phosphorus atom, an
agostic Si–H bond and a carbon atom resulting from C–H
activation of the methylene group of the starting ligand. The Si–H
bond lengths of ca. 1.70 s, as determined from X-ray data and
consistent with B3PW91 calculations on the model RuH2{g2-H–
SiMe2CH(o-C6H4)PH2}2 (5b),16 are typical of g2-H–Si bonds. The
metallated Ru–C bond lengths of ca. 2.24 s are characteristic of
Ru–C single bonds. Multinuclear NMR data highlight the unusual
coordination of the ligand. In particular, the two equivalent
Notes and references
{ CCDC 650812. For crystallographic data in CIF or other electronic
format, see DOI: 10.1039/b709408f
1 (a) W. A. G. Janowicz and R. G. Bergman, J. Am. Chem. Soc., 1982,
104, 352; (b) J. K. Hoyano and W. A. G. Graham, J. Am. Chem. Soc.,
1982, 104, 3723.
2 M. Brookhart and M. L. H. Green, J. Organomet. Chem., 1983, 250,
395.
3 G. J. Kubas, R. R. Ryan, B. I. Swanson, P. J. Vergamini and
H. J. Wasserman, J. Am. Chem. Soc., 1984, 106, 451.
4 For reviews on C–H activation, see: (a) B. A. Arndtsen, R. G. Bergman,
T. A. Mobley and T. H. Peterson, Acc. Chem. Res., 1995, 28, 154; (b)
J. A. Labinger and J. E. Bercaw, Nature, 2002, 417, 507; (c)
agostic Si–H hydrides resonate as one triplet at 29.8 ppm (JP–H
=
9 Hz) with satellites due to coupling with silicon (JSi–H = 67 Hz).
The metallated C–H proton resonates as a broad singlet at
3964 | Chem. Commun., 2007, 3963–3965
This journal is ß The Royal Society of Chemistry 2007