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bonds, at a distance compatible with the presence of a second
platinum atom. Nevertheless, the height of this peak is only about
4 e A . This feature has been inferred as the result of the presence
ꢀꢀ3
(k) F.G.A. Stone, Inorg. Chim. Acta 50 (1981) 33e42.
in the structure, together with molecules of composition Pt(dba)3,
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solid solution. Both platinum atoms were introduced in the model,
fixing to 1.0 the population parameter of the first one and tenta-
tively adjusting the second in order to obtain about the same
thermal parameters in the refinement. As the adjusted population
parameter for the “lighter” platinum is only about 0.03, this atom
has been refined with isotropic thermal parameters. All the other
non-hydrogen atoms were refined with anisotropic thermal
parameters. Hydrogen atoms were introduced in calculated posi-
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move following the “riding” convention. Final reliability factors are
listed in Table 4.
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Acknowledgements
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This work was financially supported by Ministero dell’Università
e della Ricerca Universitaria (MIUR), Progetti di Ricerca di Rilevante
Interesse Nazionale (PRIN 2007). We thank Chimet S.p.A., I-52041
Badia al Pino (Arezzo), for a loan of platinum.
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Appendix A. Supplementary material
CCDC No. 798262 contains crystallographic data for the struc-
tural analysis of compound 8. These data can be obtained free of
charge from The Cambridge Crystallographic Data Centre via www.
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