E. Ihara et al. / Journal of Organometallic Chemistry 569 (1998) 147–157
157
tors for non-hydrogen atoms for complex 2 are listed in
Table 6.
The solution was evaporated to dryness and hexane
(120 ml) was added to the residual orange powder.
After stirring for 3 h, the hexane soluble part was
concentrated to give the desired [2,6-(cyclo-C6H11–O)2-
C6H3]3Sm (0.7 g). The hexane insoluble part was dis-
solved in toluene (50 ml) and after the removal of LiCl,
the solution was concentrated to give 2.1 g of [2,6-(cy-
clo-C6H11–O)2C6H3]3Sm. Combined yield, 64%. 1H
NMR (C6D6, 400 MHz, 25°C): l 1.0–2.5 (m, 60H),
4.10 (bs, 6H), 5.64 (d, 6H), 6.64 (t, 6H). Molecular
weight is determined cryoscopically in benzene, calc.
933.4. Observed 945.
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[27] teXsan: Crystal Structure Analysis Package, Molecular Structure
Corporation (1985 & 1992).
Monomer (MMA and -caprolactone, typically 100–
200 eqivalents to initiator) was injected via a syringe
into a solution of an initiator (typically 0.04 mmol) in
toluene (10 ml) with vigorous stirring at the fixed
temperature. When alkyl isocyanares were polymerized,
0.5 ml (or none) of toluene was used. After stirring for
a fixed time, the reaction mixture was quenched by the
addition of excess MeOH. The preciptated polymer was
collected and dried under vacuum.
3.9. X-ray structural determination of [2,6-(iPrO)2-
C6H3]4SmLi 2
The integrated intensity data were measured on a
Rigaku AFC-5R diffractometer with graphite-
monochromated Mo–Kh (u=0.7106A) radiation. As
complex 2 is very air-sensitive, the crystals were sealed
in a thin-walled glass capillary tube under argon atmo-
sphere. The X-ray data were collected at room temper-
ature using ꢀ-2q scan technique to a maximum 2q
value of 55.0°. The data were corrected for conven-
tional absorption, Lorentz and polarization effects.
The crystal structure was solved by the heavy-atom
method. The Sm atom was found in the Patterson map.
Successive Fourier syntheses clearly revealed the re-
maining non-hydrogen atoms. The non-hydrogen
atoms were refined anisotropically by the full-matrix
least-squares method, while the hydrogen atoms were
fixed at their standard geometries and were not refined.
All the calculations were performed using the teXsan
crystallographic software package [27]. The final atomic
co-ordinates and equivalent isotropic temperature fac-
.