Unusual Reactivities of Linear Disilanes
Organometallics, Vol. 23, No. 3, 2004 497
-78 °C, and n-butyllithium (1.25 mL, 2.0 mmol, 1.6 M in
hexanes) was added. The solution was warmed to room
temperature, whereupon a thick suspension of white precipi-
tate formed. After the reaction mixture had stirred for 1 h at
room temperature, it was again cooled to -78 °C and 1,2-
dichlorotetramethyldisilane (1.1 equiv) was added as a neat
liquid. The solution was warmed to -5 °C very slowly (for over
1 h) and stirred at -5 °C for a total of 3 h. The volatiles were
then removed under reduced pressure; the crude mixture was
taken up in a minimal amount of Et2O and filtered through a
1 × 5 cm pad of silica gel on a glass frit. Removal of the
volatiles provided the final crude product, which was further
crystallized from toluene at -5 °C to provide pure 3,4-o-
carboranylene-1,1,2,2-tetramethyl-1,2-disilacyclobutane (3) as
a colorless solid. Yield: 78% (0.762 g, 1.56 mmol).
while the remaining H atoms were calculated in idealized
positions and included in the refinement with fixed atomic
contributions. Further detailed information is given in Table
1, and selected interatomic distances and angles are given in
Tables 3 and 4, respectively.
Com p u ta tion a l Deta ils. Stationary points on the potential
energy surface were calculated using the Amsterdam Density
Functional (ADF) program, developed by Baerends et al.20,21
and vectorized by Ravenek.22 The numerical integration
scheme applied for the calculations was developed by te Velde
et al.23,24 The geometry optimization procedure was based on
the method due to Versluis and Ziegler.25 The electronic
configurations of the molecular systems were described by
double-ú STO basis sets with polarization functions for the H,
B, and C atoms, while triple-ú Slater type basis sets were
employed for the Si, P, and Pt atoms.26,27 The 1s electrons of
B and C, the 1s-2p electrons of Si and P, and the 1s-4d
electrons of Pt were treated as frozen cores. A set of auxiliary28
s, p, d, f, and g STO functions, centered on all nuclei, was used
in order to fit the molecular density and the Coulomb and
exchange potentials in each SCF cycle. Energy differences were
calculated by augmenting the local exchange-correlation po-
tential by Vosko et al.29 with Becke’s30 nonlocal exchange
corrections and Perdew’s31 nonlocal correlation corrections
(BP86). Geometries were optimized by including nonlocal
corrections at this level of theory. First-order Pauli scalar
relativistic corrections32,33 were added variationally to the total
energy for all systems. In view of the fact that all systems
investigated in this work show a large HOMO-LUMO gap, a
spin-restricted formalism was used for all calculations. No
symmetry constraints were used.
R ea ct ion of Lin ea r Bis(o-ca r b or a n yl)d isila n e 2a
w ith P t(P Et3)3. Benzene (15 mL) was added to a mixture of
Pt(PEt3)3 (0.110 g, 0.2 mmol) and 2a (0.080 g, 0.2 mmol). The
mixture was stirred for 3 h, and then the volatile compounds
were removed under reduced pressure. Extraction of the
residue with toluene (20 mL), followed by concentration of the
extract to approximately half its volume and cooling to -5 °C,
resulted in crystallization of the cyclic bis(silyl)platinum
complex 4. Yield: 75% (0.103 g, 0.15 mmol). The supernatant
was decanted and further reduced, and the residue was
chromatographed. Elution with hexane removed a UV-active
band, from which o-carborane (0.020 g, 69%) was obtained as
a white crystalline solid after evaporation in vacuo. 31P{1H}
NMR: δ 18.40 (d, 1J Pt-P ) 1695 Hz). Anal. Calcd for B10C18H52
-
Si2P2Pt: C, 31.24; H, 7.58. Found: C, 31.35; H, 7.61. Mp )
173-175 °C dec. IR (cm-1): 3120 s, 2913 w (νCH), 2647 w, 2597
s (νBH).
For 5, a procedure analogous to the preparation of 4 was
used, but starting from 2b (0.086 g, 0.2 mmol) in benzene.
Thus, 5 was crystallized from toluene at -5 °C. Yield: 2.5%
(0.004 g, 0.005 mmol). IR (cm-1): 2963 s, 2930 m, 2876 w (νCH),
2581 (νBH).
Syn th esis of 4,5-o-Ca r bor a n ylen e-1,1,2,2,3,3-h exa m eth -
yl-1,2,3-tr isilacyclopen tan e (6). A catalytic amount of lithium
metal (0.014 g, 0.02 mmol) was added to a solution of 3 (0.488
g, 1.0 mmol) in THF (20 mL), and the mixture was stirred for
1 h at 25 °C; conversion into 6, as monitored by 1H NMR
spectroscopy, was quantitative. The solvent was removed in
vacuo and the resulting solid crystallized from toluene to give
0.146 g (0.46 mmol) of colorless microcrystals (46% yield). Anal.
Calcd for B10C8H28Si3: C, 30.17; H, 8.87. Found: C, 30.06; H,
8.84. Mp: 142-144 °C. IR (cm-1): 2963 w, 2897 w (νCH), 2588
vs, 2559 s (νBH).
Rea ction of 6 w ith P h en yla cetylen e. Phenylacetylene
(0.12 mL, 1.1 mmol) and Pt(CNBut)2 (0.0055 g, 20 µmol) were
added to a solution of 6 (0.316 g, 1.0 mmol) in toluene (20 mL),
and the mixture was heated for 1 h at 110 °C; conversion into
7, as monitored by 1H NMR spectroscopy, was quantitative.
The solvent was removed in vacuo and the resulting solid crys-
tallized from toluene to give 0.335 g (0.80 mmol) of colorless
microcrystals (80% yield). Anal. Calcd for B10C16H34Si3: C,
45.68; H, 8.15. Found: C, 45.84; H, 8.18. Mp: 150-154 °C. IR
(cm-1): 3074 w, 3053 w, 3018 w, 2961 m, 2901 w (νCH), 2633
w, 2598 s, 2584 s, 2572 s, 2557 s (νBH), 1487 m (νCdC).
Cr ysta l Str u ctu r e Deter m in a tion . Crystals of 2a ,b and
4-7 were obtained from toluene, sealed in glass capillaries
under argon, and mounted on the diffractometer. Data were
collected and corrected for Lorentz and polarization effects.
Each structure was solved by the application of direct methods
using the SHELXS-96 program19a and least-squares refine-
ment using SHELXL-97.19b After anisotropic refinement of all
non-H atoms several H atom positions could be located in
difference Fourier maps. These were refined isotropically,
Ack n ow led gm en t. We are grateful to the Korea
Research Foundation (Grant No. KRF-2002-015-CP0200)
for their financial support.
Su p p or tin g In for m a tion Ava ila ble: Crystallographic
data (excluding structure factors) for the structures of 2a ,b
and 4-7 reported in this paper and listings giving optimized
geometries of the crucial structures (3, 3′, 6, and 6′) reported
(Cartesian coordinates, in Å); crystallographic data are also
available in electronic form as CIF files. This material is
OM0341146
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(b) Sheldrick, G. M. SHELXL, Program for Crystal Structure Refine-
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