K. Jurkschat, D. Dakternieks et al.
FULL PAPER
C52H120Cl8O4Si4Sn8 (2155.4): calcd. C 28.98, H 5.61; found calcd.
C 29.35, H 5.45.
12 Union Road, Cambridge CB21EZ, UK [Fax: (internat.)
ϩ 44-1223/336-033; E-mail: deposit@ccdc.cam.ac.uk].
Acknowledgments
We thank the Deutsche Forschungsgemeinschaft, the Fonds der
Chemischen Industrie and the Australian Research Council (ARC)
for financial support.
Reaction of {[R(Cl)Sn(CH2)4Sn(Cl)R]2[RЈ(Cl)Sn(CH2)4Sn(Cl)-
RЈ]2O2}2 (12,
R
Me3CCH2, RЈ
Me3SiCH2) with
RCl2Sn(CH2)4SnCl2R (3, R ؍
Me3CCH2) (NMR Spectroscopic Ex-
periment): Compound 3 (72 mg, 0.34 mmol) was added to a solu-
tion of 12 (72 mg, 0.34 mmol) in CDCl3 (2 mL). The resulting solu-
tion was heated at reflux for 3 h and a 119Sn NMR spectrum was
recorded. Ϫ 119Sn NMR (149.21 MHz, CDCl3): δ ϭ Ϫ131.4,
Ϫ113.0, Ϫ66.7, Ϫ67.5, Ϫ69.7, Ϫ82.9, Ϫ 83.5, Ϫ84.7, Ϫ85.3,
Ϫ86.1, Ϫ100 (W1/2 ϭ 600 Hz), Ϫ137.4, Ϫ138.5, Ϫ139.6, Ϫ142.4,
Ϫ144.8, Ϫ147 (W1/2 ϭ 600).
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Addition of RCl2Sn(CH2)3SnCl2R (R ؍
Me3CCH2) to a Solution of
{[R(Cl)Sn(CH2)3Sn(Cl)R]O}4 (R ؍
Me3SiCH2) (NMR Spectro-
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ϭ Me3CCH2)
(56 mg, 0.10 mmol) was added to a solution of the double ladder
(216 mg, 0.10 mmol) in CH2Cl2 (3 mL). The resulting solution was
heated at reflux for 2 h and a 119Sn NMR spectrum (149.21 MHz,
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starting materials at δ ϭ Ϫ96.1 [2J(119SnϪ117/119Sn) ϭ 67 Hz],
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[11]
[12]
Ϫ132.9 [2J(119SnϪ117/119Sn)
[RCl2Sn(CH2)3SnCl2R, R ϭ Me3CCH2].
ϭ
69 Hz] and
δ
ϭ
107.9
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from benzene were collected with a Nonius KappaCCD diffracto-
˚
meter with graphite-monochromated Mo-Kα (0.71069 A) radiation
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at 291 K. The data collection covered almost the whole sphere of
reciprocal space with 360 frames by ω-rotation (∆/ω ϭ 1°) at two
times 10 s (9) and 20 s (12) per frame. The crystal-to-detector dis-
tance was 2.7 cm (9) and 3.0 cm with a detector-θ-offset of 5° (2).
Crystal decay was monitored by repeating the initial frames at the
end of data collection. On analysis of the duplicate reflections,
there was no indication for any decay. The data were not corrected
for absorption effects. The structure was solved by direct methods
SHELXS97[25] (Sheldrick, 1990) and successive difference Fourier
syntheses. Refinement applied full-matrix least-squares methods
SHELXL97[26] (Sheldrick, 1997). Ϫ The H atoms were placed in
geometrically calculated positions using a riding model (CϪHprim.
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ink, Inorg. Chem. 1997, 36, 2023Ϫ2029.
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Received May 26, 2000
[17]
[18]
[19]
[20]
[21]
[22]
˚
˚
0.96 A, CϪHsec. 0.97 A; Haryl CϪH 0.93), and for 9 refined with a
2
˚
common isotropic temperature factor [Uiso 0.148(7) A ] and for 12
with isotropic temperature factors constrained to be 1.5 times those
of the carrier atom. Ϫ Disordered tetramethylene, tert-butyl (12),
and isobutyl (9) groups were found with occupancies of 0.3333
[C(43Ј), C(44Ј)], 0.5 [C(3), C(5), C(3Ј), C(5Ј)], and 0.6666 [C(43),
C(44)] in 12 and of 0.15 [C(32Ј)] and 0.85 [C(32)] in 9. Ϫ Atomic
scattering factors for neutral atoms and real and imaginary disper-
sion terms were taken from International Tables for X-ray Crystal-
lography.[27] The figures were created by SHELXTL[28] (Sheldrick,
1991). Crystallographic data are given in Table 3 and selected bond
lengths and angles in Table 1. Crystallographic data for the struc-
tures reported in this paper have been deposited with the Cam-
bridge Crystallographic Data Centre as supplementary publica-
tions nos. CCDC-144264 (9) and CCDC-144265 (12). Copies of
the data can be obtained free of charge on application to CCDC,
[23]
[24]
[25]
[26]
[27]
[28]
[I00217]
160
Eur. J. Inorg. Chem. 2001, 153Ϫ160