of disilanes at transition metals, especially palladium and
platinum, is a well-known process of great synthetic value.[17]
Comparatively, such an elementary step is unprecedented at
gold, although it has been suggested recently by Klinkham-
mer et al. to account for an unusual s bond metathesis process
observed within hypersilyl gold clusters.[18] Upon coordina-
tion of phosphine–disilanes to gold, we gained evidence for
À
the spontaneous oxidative addition of s-Si Si bonds at gold to
form hitherto unknown bis(silyl) gold(III) complexes.[19,20]
These experimental results are reported herein, along with
some theoretical insights.
The reaction of the diphosphine–disilane 1 with [AuCl-
(SMe2)] in dichloromethane at À788C resulted in the
formation of the bis(silyl) gold(III) complex 2 (Scheme 2).
In marked contrast with that observed with copper and silver,
Figure 1. View of complex 3 in the solid state (ellipsoids set at 50%
probability; hydrogen atoms, counteranion, and solvate molecules
omitted for clarity). Selected bond lengths [ꢂ] and angles [8]: Au–P1
2.4135(6), Au–P2 2.4176(6), Au–Si1 2.4128(6), Au–Si2 2.4213(6); P1-
Au-P2 103.63(2), Si1-Au-Si2 89.95(2), P1-Au-Si1 84.67(2), P2-Au-Si2
82.16(2).
À
silyl skeletons are positioned tail-to-tail. The Au
Si bonds (2.4128(6) and 2.4213(6) ꢀ) are slightly
longer than those observed in the few structurally
authenticated gold(I) silyl complexes (2.365 ꢀ),[24]
but still shorter than the sum of the covalent radii
(2.47 ꢀ).[25] Furthermore, the absence of residual
contact between the two silicon atoms is shown by
À
the long Si Si distance (3.4167(9) ꢀ).
À
Scheme 2. Synthesis of complexes 2 and 3 by oxidative addition of the s-Si Si bond
of the diphosphine–disilane 1 at gold.
The coordination of the diphosphine–disilane
1 to gold thus proceeds with oxidative addition of
À
the s-Si Si bond. Such a behavior has been well-
À
the s-Si Si bond is not retained but oxidatively adds to gold.
Complex 2 is not stable above À608C, but its structure was
unambiguously ascertained by multinuclear NMR spectros-
copy at low temperature. The 29Si NMR resonance signal is
shifted downfield (33.7 ppm for 2 versus À21.2 ppm for 1),
documented with palladium and platinum,[17] but is unprece-
dented with gold.[26] The ensuing bis(silyl)gold(III) complexes
2 and 3 expand the variety of silyl complexes of gold, that, to
the best of our knowledge, was limited to date to mono-
(silyl)gold(I) species.[24]
À
indicating the cleavage of the s-Si Si bond. The associated
coupling pattern (two Si P coupling constants of 121.1 and
At this stage, the paucity of such oxidative additions at
gold prompted us to assess computationally the activation of
the s-Si Si bond by exploring the potential energy surface
(PES) of the model complex 3* featuring methyl instead of
phenyl substituents at the phosphorus atoms (Figure 2).[27]
The optimized geometry for the bis(silyl)gold(III) com-
plex 3*(III) nicely reproduces that determined crystallo-
À
À
9.4 Hz) is very similar to that typically encountered in
diphosphine bis(silyl)palladium and platinum complexes,[21]
suggesting a cis arrangement of the bis(silyl) complex 2. It is
worth noting that NMR monitoring indicated the sponta-
neous formation of the bis(silyl)gold(III) complex 2 at
À808C, with no intermediate being detected along the
oxidative addition process. With the aim of improving thermal
stability and obtaining crystals suitable for X-ray diffraction
analysis, complex 2 was reacted with one equivalent of GaCl3
as a chloride abstractor. Gratifyingly, the ensuing cationic
bis(silyl)gold(III) complex 3 was isolated in 81% yield as a
stable white powder (no sign of decomposition within days at
room temperature). The 31P and 29Si NMR data for complex 3
(31P: d = 62.9 ppm and 29Si: d = 34.4 ppm, dd, JSiÀP = 121.0 and
9.2 Hz) are very close to those of 2, suggesting in both cases
strong ionic character and only a weak interaction, if any,
between the gold center and the counteranion.[22]
À
graphically (with deviations of less than 0.05 ꢀ in the key P
À
À
Au, Au Si, and Si Si distances). Another minimum was
located on the PES for the corresponding AuI isomer 3*(I). It
is less stable in energy by 11.3 kcalmolÀ1 and has a two-
coordinate linear structure without coordination of the
À
À
disilane moiety (Si Si and Au Si distances of 2.404 and
3.360 ꢀ, respectively). A transition state 3*-TS associated
À
with oxidative addition of the s-Si Si bond of 3*(I) leading to
3*(III) was also located. The geometric features indicate a
rather late transition state with advanced cleavage of the s-
Si Si bond (2.855 ꢀ), well-developed Au Si bonds (2.554 ꢀ),
and pronounced bending of the P-Au-P skeleton (1448). The
associated activation barrier is remarkably low (10.4 kcal
molÀ1) and accounts well for the spontaneous oxidative
À
À
The molecular structure of 3 was analyzed by X-ray
diffraction (Figure 1). The ionic nature of complex 3 is
apparent from the absence of significant interaction between
À
addition of the s-Si Si bond at low temperature, as observed
À
the metal center and the GaCl4 counteranion (shortest
experimentally.
Cl···Au distance 3.9759(8) ꢀ). The gold center is surrounded
by the two phosphorus and the two silicon atoms, and adopts
square-planar geometry, as expected for a gold(III) center.[23]
Consistent with the spectroscopic data, the two phosphine–
We then sought to determine how general the unusual s-
Si Si bond activation might be that is observed upon
coordination of 1 to gold and to which degree chelating
assistance facilitates the oxidative addition process. On one
À
Angew. Chem. Int. Ed. 2011, 50, 8320 –8324
ꢀ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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