A. Conde, R. Fandos, A. Otero, A. Rodríguez, P. Terreros
FULL PAPER
OC(Me)=CMe2], 1.60 [s, 3 H, OC(Me)=CMe2], 1.83 [s, 3 H, OC-
charge from The Cambridge Crystallographic Data Center via
(Me)=CMe2], 2.03 (s, 15 H, Cp*), 7.35 (m, 9 H, Ar), 7.65 (m, 6 H, www.ccdc.cam.ac.uk/data_request/cif.
Ar) ppm. 13C{1H} NMR: δ = 10.8 (Cp*), 16.6 [OC(Me)=CMe2],
17.3 [OC(Me)=CMe2], 19.2 [OC(Me)=CMe2], 107.5 [OC(Me)=
CMe2], 119.7 (Cp*), 127.9 (Ar), 129.9 (Ar), 135.4 (Ar), 136.5
(Aripso), 146.5 [OC(Me)=CMe2] ppm. C33H39O3SiTa·0.7C7H8
Acknowledgments
(757.23): calcd. C 60.12, H 5.93; found C 60.24, H 5.84.
We gratefully acknowledge financial support from the Dirección
General de Investigación (MEC), Spain (project CTQ2005-08123-
C02-01/BQU) and the Junta de Comunidades de Castilla-La Man-
cha, Spain (project PBI05-023).
Synthesis of [TaCp*Me2(OSiPh3)][MeB(C6F5)3] (6): A solution of
B(C6F5)3 (0.075g, 0.147 mmol) in toluene (10 mL) was added to
a solution of [TaCp*Me3(OSiPh3)] (0.94g, 0.147 mmol) in toluene
(15 mL) at room temperature. The oil formed after 5 min was sepa-
rated from the solution and characterized as complex 6 (yield
0.112 g, 67%). 1H NMR (CDCl3, room temp.): δ = 0.34 (br. s, 3
H, MeB), 0.90 (s, 6 H, Ta-Me), 1.89 (s, 15 H, Cp*), 7.43 (m, 15 H,
Ar) ppm. 13C{1H} NMR: δ = 11.7 (B-Me), 11.82 (Cp*), 77.7 (Ta-
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Me), 126.8 (Cp*), 129.6 (Ar), 131.4 (Ar), 132.8 (Ar), 135.5 (Aripso
)
ppm. 19F NMR: δ = –132.6 (m, 6 F), –164.8 (m, 3 F), –167.3 (m,
6 F) ppm.
X-ray Structure Determination for 2: Crystals of 2 were obtained
from pentane. Data were collected with a Bruker X8 APEX II
CCD-based diffractometer equipped with a graphite-monochro-
mated Mo-Kα radiation source (λ = 0.71073 Å). The crystal data,
data collection, structural solution, and refinement parameters are
summarized in Table 2. Data were integrated using SAINT[20] and
an absorption correction was performed with the program SAD-
ABS.[21] The structure was solved by direct methods using
SHELXTL,[22] and refined by full-matrix least-squares methods
based on F2. All non-hydrogen atoms were refined with anisotropic
thermal parameters. Hydrogen atoms were placed using a “riding
model” and included in the refinement at calculated positions. The
large residual electron density is probably due to the poor quality
of the crystals. CCDC-673906 contains the supplementary crystal-
lographic data for this paper. These data can be obtained free of
Table 2. Crystal data and structure refinement for 2.
Empirical formula
Formula mass
C40H48NOSiTa
767.83
Temperature [K]
Wavelength [Å]
180(2)
0.71073
Crystal system
Space group
triclinic
P1
¯
a [Å]
b [Å]
c [Å]
α [°]
9.6650(5)
12.8440(7)
16.5020(9)
67.348(3)
β [°]
86.194(3)
68.956(3)
1758.2(2)
γ [°]
Volume [Å3]
Z
2
Density (calculated) [gcm–3]
Absorption coefficient [mm–1]
F(000)
1.450
3.191
780
Crystal size [mm]
θ range for data collection [°]
Index ranges
0.14ϫ0.11ϫ0.09
1.34–26.45
–12ՅhՅ11
–16ՅkՅ16
–20ՅlՅ20
23496
Reflections collected
Independent reflections
Data/restraints/parameters
Goodness-of-fit on F2
Final R indices [I Ͼ 2σ(I)]
Largest diff. peak/hole
7212 [R(int) = 0.1092]
7212/0/407
0.963
R1 = 0.0579, wR2 = 0.1107
2.149/–1.234
3066
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Eur. J. Inorg. Chem. 2008, 3062–3067