L.D. Field et al. / Polyhedron 25 (2006) 1498–1506
1505
values for Df0 and Df00 were those of Creagh and McAuley
[35]. The values for the mass attenuation coefficients were
those of Creagh and Hubbell [36]. The structure was solved
in the space group P21/n (#14) by heavy-atom Patterson
methods [37] and expanded using Fourier techniques [38].
In general non-hydrogen atoms were modelled anisotropi-
cally, however C(3), C(5), C(17), C(18), C(30) and C(35)
were refined with isotropic thermal parameters. Hydrogen
atoms were included in the model at calculated positions
with group thermal parameters. ORTEP projections of
the molecule are provided in Figs. 2 and 3 [39].
in the space group P21/n (#14) by direct methods [40] and
expanded using Fourier techniques [38]. Non-hydrogen
atoms were modeled with anisotropic thermal parameters
and hydrogen atoms were included in the model at calcu-
lated positions with group thermal parameters. ORTEP
projections of the molecule are provided in Figs. 1 and 2
[39].
4.6. Crystal data for [Mn(g5-C5Ph5)(CO)2(PMe2Ph)]
(2)
Formula C45H33MnO2P, M 691.62, monoclinic, space
4.5. Crystal data for [Mn(g5-C5Ph5)(CO)3] (1)
group P21/n(#14), a 15.251(4), b 13.804(3), c 17.682(4) A,
˚
3
b 106.39(2), V 3571.2(15) A , Dc 1.286 g cmꢀ3, Z 4, crystal
˚
Formula C38H25MnO3, M 584.52, monoclinic, space
size 0.28 by 0.25 by 0.11 mm, colour yellow, habit blade,
˚
˚
group P21/n (#14), a 16.929(4), b 8.928(2), c 20.054(4) A, b
temperature 294(2) K, k(Cu Ka) 1.5418 A, l(Cu Ka)
3
106.04(2), V 2913.0(11) A , Dc 1.333 g cmꢀ3, Z 4, crystal size
3.714 mmꢀ1
, T(Analytical)min,max 0.420, 0.698, 2hmax
˚
0.47 by 0.20 by 0.12 mm, colour yellow, habit blade, temper-
130.20, hkl range 0 17, 0 16, ꢀ20 19, N 6028, Nind 6027
(Rmerge 0.05469), Nobs 4016(I > 2r(I)), Nvar 443, residuals6
R1(F) 0.0472, wR2ꢀ(F32) 0.1356, GoF(all) 1.189, Dqmin,max
˚
ature 294(2) K, k(Mo Ka) 0.71073 A, l(Mo Ka)
0.4900 mmꢀ1, T (Analytical)min,max 0.8984, 0.9489, 2hmax
49.98, hkl range ꢀ20 19, ꢀ1 10, ꢀ1 10, N 4061, Nind 3167-
(Rmerge 0.0738), Nobs 2058(I > 2r(I)), Nvar 344, residuals5
R1(F) 0.0967, wR2ꢀ(F32) 0.2971, GoF(all) 1.274, Dqmin,max
ꢀ
˚
ꢀ0.383, 0.495 e A
.
Acknowledgement
ꢀ
˚
ꢀ1.516, 1.455 e A
.
[Mn(g5-C5Ph5)(CO)2(PMe2Ph)] (2): a yellow blade like
crystal having approximate dimensions of 0.28 · 0.25 ·
0.11 mm was attached to a thin glass fibre, and mounted
on a Rigaku AFC7R diffractometer employing graphite
monochromated Cu Ka radiation from a rotating anode
generator. Primitive monoclinic cell constants were
obtained from a least-squares refinement using the setting
angles of 21 reflections in the range 68.01 < 2h < 91.99ꢁ.
Diffraction data were collected at a temperature of
21 1 ꢁC using x–2h scans to a maximum 2h value of
130.2ꢁ. Omega scans of several intense reflections made
prior to data collection, had an average width at half-
height of 0.18ꢁ, and scans of (1.73 + 0.35 tan h)ꢁ were made
at a speed of 16.0ꢁ/min (in omega). The weak reflections
(I < 15.0r(I)) were rescanned up to 10 times. Stationary
background counts were recorded on each side of the
reflection, with a 2:1 ratio of peak to background counting
time. The intensities of three representative reflections
measured every 150 reflections, did not change significantly
during the data collection. An analytical absorption correc-
tion was applied and the data were also corrected for
Lorentz and polarisation effects.
We thank the Australian Research Council for financial
support.
References
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¨
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345.
All calculations were undertaken with the TEXSAN [32]
crystallographic software package. Neutral atom scattering
factors were taken from Cromer and Waber [33]. Anoma-
lous dispersion effects were included in Fcalc [34] and the
values for Df0 and Df00 were those of Creagh and McAuley
[35]. The values for the mass attenuation coefficients were
those of Creagh and Hubbell [36]. The structure was solved
[15] G. Wilkinson, F.G.A. Stone, E.W. Abel (Eds.), Comprehensive
Organometallic Chemistry, vol. 6, Pergamon, 1995, p. 109.
[16] F.P.A. Johnson, M.W. George, V.N. Bagratashvili, L.N. Vereshcha-
gina, M. Poliakoff, Mendeleev Commun. (1991) 26.
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283.
[18] L.D. Field, T.W. Hambley, P.A. Humphrey, A.F. Masters, P.
Turner, Polyhedron 17 (1998) 2587.
P
P
P
P
P
P
2
2
5
6
R1 ¼ kF oj ꢀ jF ck= jF oj for F o > 2rðF oÞ; wR2 ¼ ð wðF 2o ꢀ F c2Þ =
R1 ¼ kF oj ꢀ jF ck= jF oj for F o > 2rðF oÞ; wR2 ¼ ð wðF 2o ꢀ F c2Þ =
P
P
2
1=2
2
2
1=2
2
ðwF 2c Þ Þ all reflections w ¼ 1=½r2ðF 2oÞ þ ð0:10PÞ þ 15:0Pꢁ where P ¼
ðwF 2cÞ Þ all reflections w ¼ 1=½r2ðF 2oÞ þ ð0:05PÞ þ 1:0Pꢁ where P ¼
ðF 2o þ 2F 2c Þ=3.
ðF 2o þ 2F 2c Þ=3.